Abstract

Linear skew products of the complex plane, \begin{document}$ \left. \begin{array}{rcl} \theta & \mapsto & \theta+\omega,\\ z & \mapsto & a(\theta)z, \end{array} \right\} $\end{document} where $ \theta\in {\mathbb T} $, $ z\in {\mathbb C} $, $ \frac{\omega}{2\pi} $ is irrational, and $ \theta\mapsto a(\theta) \in {\mathbb C}\setminus \{0\} $ is a smooth map, appear naturally when linearizing dynamics around an invariant curve of a quasi-periodically forced complex map. In this paper we study linear and topological equivalence classes of such maps through conjugacies which preserve the skewed structure, relating them to the Lyapunov exponent and the winding number of $ \theta\mapsto a(\theta) $. We analyze the transition between these classes by considering one parameter families of linear skew products. Finally, we show that, under suitable conditions, an affine variation of the maps above has a non-reducible invariant curve that undergoes a fractalization process when the parameter goes to a critical value. This phenomenon of fractalization of invariant curves is known to happen in nonlinear skew products, but it is remarkable that it also occurs in simple systems as the ones we present.

Highlights

  • In this work we are concerned with the dynamics of linear skew products of the complex plane

  • The simplest dynamics is the one given by the class of reducible skew products, which are those that can be reduced to a linear system with constant coefficients, under a linear change of variables

  • We show that any linear system can be written, via a linear change, as θ → θ + ω, z → beimωeinθz, where n = wind(a, 0), m is an arbitrary integer, b ∈ C and log |b| is the Lyapunov exponent

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Summary

Introduction

In this work we are concerned with the dynamics of linear skew products of the complex plane. The simplest dynamics is the one given by the class of reducible skew products, which are those that can be reduced to a linear system with constant coefficients, under a linear change of variables (see Section 2). In this context, we show (Corollary 3.8) that reducibility can be characterized by the winding number being equal to zero. Note that the linearization of the dynamics at the invariant curve (which in this case is just the linear part of the system) is non-reducible The same phenomenon happens when μ approaches 1 from above, but the invariant curve is repelling

Preliminaries
Linear invertible skew-products
Linear conjugacy classes
Topological conjugacy classes
Normal forms and Lyapunov exponents
A fractalization mechanism
Asymptotic behaviour
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