Rotation numbers for quasi-periodically forced monotone circle maps

Rotation numbers have played a central role in the study of (unforced) monotone circle maps. In such a case it is possible to obtain a priori bounds of the form - 1/n h (1/n)(yn - y 0) h + 1/n, where (1/n)(yn - y 0) is an estimate of the rotation number obtained from an orbit of length n with initial condition y 0, and is the true rotation number. This allows rotation numbers to be computed reliably and efficiently. Although Herman has proved that quasi-periodically forced circle maps also possess a well-defined rotation number, independent of initial condition, the analogous bound does not appear to hold. In particular, two of the authors have recently given numerical evidence that there exist quasi-periodically forced circle maps for which y n - y 0 - n is not bounded. This renders the estimation of rotation numbers for quasi-periodically forced circle maps much more problematical. In this paper, a new characterization of the rotation number is derived for quasiperiodically forced circle maps based upon integrating iterates of an arbitrary smooth curve. This satisfies analogous bounds to above and permits us to develop improved numerical techniques for computing the rotation number. Additionally, the boundedness of yn - y 0 - n is considered. It is shown that if this quantity is bounded (both above and below) for one orbit, then it is bounded for all orbits. Conversely, if for any orbit yn - y 0 - n is unbounded either above or below, then there is a residual set of orbits for which yn - y 0 - n is unbounded both above and below. In proving these results a min-max characterization of the rotation number is also presented. The performance of an algorithm based on this is evaluated, and on the whole it is found to be inferior to the integral based method.

[1]  L. Arnold Random Dynamical Systems , 2003 .

[2]  R. Sturman Strange nonchaotic attractors in quasiperiodically forced systems , 2001 .

[3]  Arkady Pikovsky,et al.  The structure of mode-locked regions in quasi-periodically forced circle maps , 2000 .

[4]  Rob Sturman,et al.  Semi-uniform ergodic theorems and applications to forced systems , 2000 .

[5]  Rob Sturman,et al.  Scaling of intermittent behaviour of a strange nonchaotic attractor , 1999 .

[6]  Celso Grebogi,et al.  Phase-locking in quasiperiodically forced systems , 1997 .

[7]  J. Stark Invariant graphs for forced systems , 1997 .

[8]  Jürgen Kurths,et al.  Strange non-chaotic attractor in a quasiperiodically forced circle map , 1995 .

[9]  J. Stark,et al.  Locating bifurcations in quasiperiodically forced systems , 1995 .

[10]  A. Katok,et al.  Introduction to the Modern Theory of Dynamical Systems: INTRODUCTION , 1995 .

[11]  Wojciech Słomczyński Continuous subadditive processes and formulae for Lyapunov characteristic exponents , 1995 .

[12]  F. Rhodes,et al.  Topologies and Rotation Numbers for Families of Monotone Functions on the Circle , 1991 .

[13]  Mingzhou Ding,et al.  Dimensions of strange nonchaotic attractors , 1989 .

[14]  Grebogi,et al.  Evolution of attractors in quasiperiodically forced systems: From quasiperiodic to strange nonchaotic to chaotic. , 1989, Physical review. A, General physics.

[15]  J. Luck,et al.  Quasiperiodicity and types of order; a study in one dimension , 1987 .

[16]  F. Rhodes,et al.  Rotation Numbers for Monotone Functions on the Circle , 1986 .

[17]  M. R. Herman Une méthode pour minorer les exposants de Lyapounov et quelques exemples montrant le caractère local d’un théorème d’Arnold et de Moser sur le tore de dimension 2 , 1983 .

[18]  Vladimir Igorevich Arnold,et al.  Geometrical Methods in the Theory of Ordinary Differential Equations , 1983 .

[19]  Subadditive mean ergodic theorems , 1981, Ergodic Theory and Dynamical Systems.

[20]  M. R. Herman Sur la Conjugaison Différentiable des Difféomorphismes du Cercle a des Rotations , 1979 .

[21]  P. Davis,et al.  Methods of Numerical Integration , 1985 .

[22]  A Uniform Ergodic Theorem , 1965 .