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Volumn 57, Issue 6, 1998, Pages 6577-6588

Calculating topological entropy for transient chaos with an application to communicating with chaos

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EID: 0000621770     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.57.6577     Document Type: Article
Times cited : (20)

References (22)
  • 2
    • 0003582543 scopus 로고
    • Cambridge University Press, Cambridge, England, and appropriate references therein
    • E. Ott, Chaos in Dynamical Systems (Cambridge University Press, Cambridge, England, 1993), and appropriate references therein.
    • (1993) Chaos in Dynamical Systems
    • Ott, E.1
  • 15
    • 43949161715 scopus 로고
    • A method similar to that of Newhouse and Pignataro but applied to a chaotic saddle in a physical situation (motion of tracer particles in a fluid flow) can be found in E. M. Ziemniak, C. Jung, and T. Tél, Physica D 76, 123 (1994).
    • (1994) Physica D , vol.76 , pp. 123
    • Ziemniak, E.M.1    Jung, C.2    Tél, T.3
  • 22
    • 84957340500 scopus 로고
    • This paper considers the parameter dependence of the entropy of a chaotic attractor. As the parameter increases, more orbits are forbidden, pruned. At the onset of pruning, i.e., the critical parameter beyond which orbits in the chaotic attractor are forbidden, it is shown that the decrease of the topological entropy satisfies a power law behavior. The scaling exponent is shown to be the pointwise dimension of the first pruned orbit. For the one-dimensional map we consider here, pruning starts as soon as the size of the gap is strictly positive. Since the pointwise dimension of any point on the original attractor is one, the scaling exponent should be one as well. This is clearly the case in Eq. (41). EULEEJ
    • This is consistent with J. Vollmer and W. Breymann, Europhys. Lett. 27, 23 (1994). This paper considers the parameter dependence of the entropy of a chaotic attractor. As the parameter increases, more orbits are forbidden, pruned. At the onset of pruning, i.e., the critical parameter beyond which orbits in the chaotic attractor are forbidden, it is shown that the decrease of the topological entropy satisfies a power law behavior. The scaling exponent is shown to be the pointwise dimension of the first pruned orbit. For the one-dimensional map we consider here, pruning starts as soon as the size of the gap is strictly positive. Since the pointwise dimension of any point on the original attractor is one, the scaling exponent should be one as well. This is clearly the case in Eq. (41). EULEEJ
    • (1994) Europhys. Lett. , vol.27 , pp. 23
    • Vollmer, J.1    Breymann, W.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.