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Upper, down, two-sided Lorenz attractor, collisions, merging, and switching

Published online by Cambridge University Press:  21 February 2024

DIEGO BARROS
Affiliation:
Instituto de Matemática, Universidade Federal do Rio de Janeiro, Rio de Janeiro, Brazil (e-mail: diegosbarros@macae.ufrj.br)
CHRISTIAN BONATTI
Affiliation:
Institut de Mathématiques de Bourgogne, CNRS, Université de Bourgogne, Dijon, France (e-mail: bonatti@u-bourgogne.fr)
MARIA JOSÉ PACIFICO*
Affiliation:
Instituto de Matemática, Universidade Federal do Rio de Janeiro, Rio de Janeiro, Brazil (e-mail: diegosbarros@macae.ufrj.br)

Abstract

We present a modified version of the well-known geometric Lorenz attractor. It consists of a $C^1$ open set ${\mathcal O}$ of vector fields in ${\mathbb R}^3$ having an attracting region ${\mathcal U}$ satisfying three properties. Namely, a unique singularity $\sigma $; a unique attractor $\Lambda $ including the singular point and the maximal invariant in ${\mathcal U}$ has at most two chain recurrence classes, which are $\Lambda $ and (at most) one hyperbolic horseshoe. The horseshoe and the singular attractor have a collision along with the union of $2$ codimension $1$ submanifolds which split ${\mathcal O}$ into three regions. By crossing this collision locus, the attractor and the horseshoe may merge into a two-sided Lorenz attractor, or they may exchange their nature: the Lorenz attractor expels the singular point $\sigma $ and becomes a horseshoe, and the horseshoe absorbs $\sigma $ becoming a Lorenz attractor.

Type
Original Article
Copyright
© The Author(s), 2024. Published by Cambridge University Press

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