2014
DOI: 10.3934/jcd.2014.1.307
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Lattice structures for attractors I

Abstract: ABSTRACT. We describe the basic lattice structures of attractors and repellers in dynamical systems. The structure of distributive lattices allows for an algebraic treatment of gradient-like dynamics in general dynamical systems, both invertible and noninvertible. We separate those properties which rely solely on algebraic structures from those that require some topological arguments, in order to lay a foundation for the development of algorithms to manipulate these structures computationally.

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Cited by 32 publications
(96 citation statements)
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References 15 publications
(21 reference statements)
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“…To address the lack of robustness of invariant sets with respect to parameters, another change in perspective is needed. Initiated by C. Conley [37] and developed over the last 40 years [38][39][40][41] the emphasis shifts from invariant sets to positively attracting sets.…”
Section: Discussionmentioning
confidence: 99%
“…To address the lack of robustness of invariant sets with respect to parameters, another change in perspective is needed. Initiated by C. Conley [37] and developed over the last 40 years [38][39][40][41] the emphasis shifts from invariant sets to positively attracting sets.…”
Section: Discussionmentioning
confidence: 99%
“…This process can be made fairly general, see e.g. [KMV14,KMV16]. For illustration, we now outline one constructive approach that we used to produce the sample results throughout the paper.…”
Section: Computational Conley Indexmentioning
confidence: 99%
“…Further development of these methods relies on understanding the way in which lattices and order naturally play a role in dynamics on the fundamental level of attractors, repellers, and invariant sets, cf. [19]. Analogues of these basic concepts in dynamical systems theory also exist in directed graphs and are used to analyze combinatorial representations of dynamical systems.…”
mentioning
confidence: 99%
“…A subset N Ă X is an attracting block if f pcl Nq Ă int N, and ωpNq " A is the associated attractor, cf. [19,20]. In many cases attracting blocks are readily computable, while the lattice of attractors is not directly computable in general.…”
mentioning
confidence: 99%
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