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2
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0003582543
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Cambridge University Press, Cambridge, England, and appropriate references therein
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E. Ott, Chaos in Dynamical Systems (Cambridge University Press, Cambridge, England, 1993), and appropriate references therein.
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(1993)
Chaos in Dynamical Systems
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Ott, E.1
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15
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43949161715
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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).
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(1994)
Physica D
, vol.76
, pp. 123
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Ziemniak, E.M.1
Jung, C.2
Tél, T.3
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20
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12044256754
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S. Hayes, C. Grebogi, E. Ott, and A. Mark, Phys. Rev. Lett. 73, 1781 (1994).
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(1994)
Phys. Rev. Lett.
, vol.73
, pp. 1781
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Hayes, S.1
Grebogi, C.2
Ott, E.3
Mark, A.4
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22
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84957340500
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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
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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
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(1994)
Europhys. Lett.
, vol.27
, pp. 23
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Vollmer, J.1
Breymann, W.2
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