2020
DOI: 10.1063/5.0007230
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Kantorovich–Rubinstein–Wasserstein distance between overlapping attractor and repeller

Abstract: We consider several examples of dynamical systems demonstrating overlapping attractor and repeller. These systems are constructed via introducing controllable dissipation to prototypic models with chaotic dynamics (Anosov cat map, Chirikov standard map, and incompressible three-dimensional flow of the ABC-type on a three-torus) and ergodic non-chaotic behavior (skew-shift map). We employ the Kantorovich–Rubinstein–Wasserstein distance to characterize the difference between the attractor and the repeller, in de… Show more

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Cited by 20 publications
(3 citation statements)
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“…Small perturbations do not destroy the hyperbolicity of map (11). As an example, we consider the two-dimensional map from [28]:…”
Section: Two-dimensional Mapsmentioning
confidence: 99%
“…Small perturbations do not destroy the hyperbolicity of map (11). As an example, we consider the two-dimensional map from [28]:…”
Section: Two-dimensional Mapsmentioning
confidence: 99%
“…Also, we calculate the Kantorovich-Rubinstein-Wasserstein distance (KRWD) between the chaotic attractor and the chaotic repeller, which reflects the degree of similarity of the attractor and repeller as sets [43]. We calculate the KRWD using a free available program code [44].…”
Section: Methodsmentioning
confidence: 99%
“…There are some primary tools which can be utilized to study the existence of these invariant measures such as Gibbs and SBR measures [53]- [55]. The discrete approximation of the invariant measures has been provided in several works, see for example [56]- [58] and references there in.…”
Section: Proximity Of Ghost and Non-stationary Attractorsmentioning
confidence: 99%