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Palmero MS, Caldas IL, Sokolov IM. Finite-time recurrence analysis of chaotic trajectories in Hamiltonian systems. CHAOS (WOODBURY, N.Y.) 2022; 32:113144. [PMID: 36456326 DOI: 10.1063/5.0102424] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/09/2022] [Accepted: 11/01/2022] [Indexed: 06/17/2023]
Abstract
In this work, we show that a finite-time recurrence analysis of different chaotic trajectories in two-dimensional non-linear Hamiltonian systems provides useful prior knowledge of their dynamical behavior. By defining an ensemble of initial conditions, evolving them until a given maximum iteration time, and computing the recurrence rate of each orbit, it is possible to find particular trajectories that widely differ from the average behavior. We show that orbits with high recurrence rates are the ones that experience stickiness, being dynamically trapped in specific regions of the phase space. We analyze three different non-linear maps and present our numerical observations considering particular features in each of them. We propose the described approach as a method to visually illustrate and characterize regions in phase space with distinct dynamical behaviors.
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Affiliation(s)
- Matheus S Palmero
- Instituto de Física, Universidade de São Paulo, São Paulo, SP, Brazil
| | - Iberê L Caldas
- Instituto de Física, Universidade de São Paulo, São Paulo, SP, Brazil
| | - Igor M Sokolov
- Institut für Physik, Humboldt-Universität zu Berlin, Berlin, Germany
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Zhokh A, Strizhak P. Non-Fickian Transport in Porous Media: Always Temporally Anomalous? Transp Porous Media 2018. [DOI: 10.1007/s11242-018-1066-6] [Citation(s) in RCA: 10] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/18/2023]
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Livorati ALP, Kroetz T, Dettmann CP, Caldas IL, Leonel ED. Transition from normal to ballistic diffusion in a one-dimensional impact system. Phys Rev E 2018; 97:032205. [PMID: 29776143 DOI: 10.1103/physreve.97.032205] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/17/2017] [Indexed: 11/07/2022]
Abstract
We characterize a transition from normal to ballistic diffusion in a bouncing ball dynamics. The system is composed of a particle, or an ensemble of noninteracting particles, experiencing elastic collisions with a heavy and periodically moving wall under the influence of a constant gravitational field. The dynamics lead to a mixed phase space where chaotic orbits have a free path to move along the velocity axis, presenting a normal diffusion behavior. Depending on the control parameter, one can observe the presence of featured resonances, known as accelerator modes, that lead to a ballistic growth of velocity. Through statistical and numerical analysis of the velocity of the particle, we are able to characterize a transition between the two regimes, where transport properties were used to characterize the scenario of the ballistic regime. Also, in an analysis of the probability of an orbit to reach an accelerator mode as a function of the velocity, we observe a competition between the normal and ballistic transport in the midrange velocity.
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Affiliation(s)
- André L P Livorati
- Departamento de Física, UNESP, Universidade Estadual Paulista, Av. 24A 1515, Bela Vista, 13506-900, Rio Claro, SP, Brazil.,School of Mathematics, University of Bristol, Bristol, BS8 1TW, United Kingdom
| | - Tiago Kroetz
- Departamento Acadêmico de Física, Universidade Tecnológica Federal do Paraná UTFPR, Campus Pato Branco, 85503-390, Pato Branco, PR, Brazil
| | - Carl P Dettmann
- School of Mathematics, University of Bristol, Bristol, BS8 1TW, United Kingdom
| | - Iberê L Caldas
- Instituto de Física, IFUSP, Universidade de São Paulo, USP Rua do Matão Tr.R 187, Cidade Universitária, 05314-970, São Paulo, SP, Brazil
| | - Edson D Leonel
- Departamento de Física, UNESP, Universidade Estadual Paulista, Av. 24A 1515, Bela Vista, 13506-900, Rio Claro, SP, Brazil
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Ryzhov EA. Nonlinear dynamics of an elliptic vortex embedded in an oscillatory shear flow. CHAOS (WOODBURY, N.Y.) 2017; 27:113101. [PMID: 29195330 DOI: 10.1063/1.4996769] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
The nonlinear dynamics of an elliptic vortex subjected to a time-periodic linear external shear flow is studied numerically. Making use of the ideas from the theory of nonlinear resonance overlaps, the study focuses on the appearance of chaotic regimes in the ellipse dynamics. When the superimposed flow is stationary, two general types of the steady-state phase portrait are considered: one that features a homoclinic separatrix delineating bounded and unbounded phase trajectories and one without a separatrix (all the phase trajectories are bounded in a periodic domain). When the external flow is time-periodic, the ensuing nonlinear dynamics differs significantly in both cases. For the case with a separatrix and two distinct types of phase trajectories: bounded and unbounded, the effect of the most influential nonlinear resonance with the winding number of 1:1 is analyzed in detail. Namely, the process of occupying the central stability region associated with the steady-state elliptic critical point by the stability region associated with the nonlinear resonance of 1:1 as the perturbation frequency gradually varies is investigated. A stark increase in the persistence of the central regular dynamics region against perturbation when the resonance of 1:1 associated stability region occupies the region associated with the steady-state elliptic critical point is observed. An analogous persistence of the regular motion occurs for higher perturbation frequencies when the corresponding stability islands reach the central stability region associated with the steady-state elliptic point. An analysis for the case with the resonance of 1:2 is presented. For the second case with only bounded phase trajectories and, therefore, no separatrix, the appearance of much bigger stability islands associated with nonlinear resonances compared with the case with a separatrix is reported.
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Affiliation(s)
- Eugene A Ryzhov
- Pacific Oceanological Institute of FEB RAS, 43, Baltiyskaya Street, Vladivostok 690041, Russia
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