Anti-Integrability for 3-Dimensional Quadratic Maps

TL;DR

This paper explores the dynamics of three-dimensional quadratic maps using the anti-integrable limit concept, revealing symbolic dynamics, bifurcations, and complex orbit structures through contraction and numerical methods.

Contribution

It introduces a novel application of the anti-integrable limit to 3D quadratic maps, analyzing symbolic dynamics and orbit continuation in different geometric cases.

Findings

Parameter domains for unique AI states identified

Bifurcation structures and horseshoe-like orbits computed

Conjecture on symbol sequences differing in one position

Abstract

We study the dynamics of the three-dimensional quadratic diffeomorphism using a concept first introduced thirty years ago for the Frenkel-Kontorova model of condensed matter physics: the anti-integrable (AI) limit. At the traditional AI limit, orbits of a map degenerate to sequences of symbols and the dynamics is reduced to the shift operator, a pure form of chaos. Under nondegeneracy conditions, a contraction mapping argument can show that infinitely many AI states continue to orbits of the deterministic map. For the 3D quadratic map, the AI limit that we study is a quadratic correspondence whose branches, a pair of one-dimensional maps, introduce symbolic dynamics on two symbols. The AI states, however, are nontrivial orbits of this correspondence. The character of these orbits depends on whether the quadratic takes the form of an ellipse, a hyperbola, or a pair of lines. Using contraction arguments, we find parameter domains for each case such that each symbol sequence corresponds to a unique AI state. In some parameter domains, sufficient conditions are then found for each such AI state to continue away from the limit to become an orbit of the original 3D map. Numerical continuation methods extend these results, allowing computation of bifurcations and obtaining orbits with horseshoe-like structures and intriguing self-similarity. We conjecture that pairs of periodic orbits in saddle-node or period doubling bifurcations have symbol sequences that differ in exactly one position.