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Covariant Lyapunov vectors for rigid disk systems

We carry out extensive computer simulations to study the Lyapunov instability of a two-dimensional hard-disk system in a rectangular box with periodic boundary conditions. The system is large enough to allow the formation of Lyapunov modes parallel to the x-axis of the box. The Oseledec splitting in...

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Detalles Bibliográficos
Autores principales: Bosetti, Hadrien, Posch, Harald A.
Formato: Texto
Lenguaje:English
Publicado: North Holland Publishing 2010
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2982751/
https://www.ncbi.nlm.nih.gov/pubmed/21151326
http://dx.doi.org/10.1016/j.chemphys.2010.06.010
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author Bosetti, Hadrien
Posch, Harald A.
author_facet Bosetti, Hadrien
Posch, Harald A.
author_sort Bosetti, Hadrien
collection PubMed
description We carry out extensive computer simulations to study the Lyapunov instability of a two-dimensional hard-disk system in a rectangular box with periodic boundary conditions. The system is large enough to allow the formation of Lyapunov modes parallel to the x-axis of the box. The Oseledec splitting into covariant subspaces of the tangent space is considered by computing the full set of covariant perturbation vectors co-moving with the flow in tangent space. These vectors are shown to be transversal, but generally not orthogonal to each other. Only the angle between covariant vectors associated with immediate adjacent Lyapunov exponents in the Lyapunov spectrum may become small, but the probability of this angle to vanish approaches zero. The stable and unstable manifolds are transverse to each other and the system is hyperbolic.
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spelling pubmed-29827512010-12-06 Covariant Lyapunov vectors for rigid disk systems Bosetti, Hadrien Posch, Harald A. Chem Phys Article We carry out extensive computer simulations to study the Lyapunov instability of a two-dimensional hard-disk system in a rectangular box with periodic boundary conditions. The system is large enough to allow the formation of Lyapunov modes parallel to the x-axis of the box. The Oseledec splitting into covariant subspaces of the tangent space is considered by computing the full set of covariant perturbation vectors co-moving with the flow in tangent space. These vectors are shown to be transversal, but generally not orthogonal to each other. Only the angle between covariant vectors associated with immediate adjacent Lyapunov exponents in the Lyapunov spectrum may become small, but the probability of this angle to vanish approaches zero. The stable and unstable manifolds are transverse to each other and the system is hyperbolic. North Holland Publishing 2010-10-05 /pmc/articles/PMC2982751/ /pubmed/21151326 http://dx.doi.org/10.1016/j.chemphys.2010.06.010 Text en © 2010 Elsevier B.V. https://creativecommons.org/licenses/by-nc-nd/3.0/ Open Access under CC BY-NC-ND 3.0 (https://creativecommons.org/licenses/by-nc-nd/3.0/) license
spellingShingle Article
Bosetti, Hadrien
Posch, Harald A.
Covariant Lyapunov vectors for rigid disk systems
title Covariant Lyapunov vectors for rigid disk systems
title_full Covariant Lyapunov vectors for rigid disk systems
title_fullStr Covariant Lyapunov vectors for rigid disk systems
title_full_unstemmed Covariant Lyapunov vectors for rigid disk systems
title_short Covariant Lyapunov vectors for rigid disk systems
title_sort covariant lyapunov vectors for rigid disk systems
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2982751/
https://www.ncbi.nlm.nih.gov/pubmed/21151326
http://dx.doi.org/10.1016/j.chemphys.2010.06.010
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