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Basin bifurcation in quasiperiodically forced systems

Ulrike Feudel1, Annette Witt1, Ying-Cheng Lai2, and Celso Grebogi1,3

  • 1Institut für Physik, Universität Potsdam, Am Neuen Palais, PF 601553, D-14415, Potsdam, Germany
  • 2Departments of Physics and Astronomy and of Mathematics, The University of Kansas, Lawrence, Kansas 66045
  • 3Institute for Plasma Research, University of Maryland, College Park, Maryland 20742

Phys. Rev. E 58, 3060 – Published 1 September, 1998

DOI: https://doi.org/10.1103/PhysRevE.58.3060

Abstract

In this paper we study quasiperiodically forced systems exhibiting fractal and Wada basin boundaries. Specifically, by utilizing a class of representative systems, we analyze the dynamical origin of such basin boundaries and we characterize them. Furthermore, we find that basin boundaries in a quasiperiodically driven system can undergo a unique type of bifurcation in which isolated “islands” of basins of attraction are created as a system parameter changes. The mechanism for this type of basin boundary bifurcation is elucidated.

References (29)

  1. C. Grebogi, S. W. McDonald, E. Ott, and J. A. Yorke, Phys. Lett. 99A, 415 (1983).
  2. S. W. McDonald, C. Grebogi, E. Ott, and J. A. Yorke, Physica D 17, 125 (1985).
  3. F. C. Moon, Phys. Rev. Lett. 53, 962 (1984); ibid.F. C. Moon and G. -X. Li, 55, 1439 (1985).
  4. C. Grebogi, H. E. Nusse, E. Ott, and J. A. Yorke, in Dynamical Systems, edited by J. C. Alexander, Lecture Notes in Mathematics Vol. 1342 (Springer-Verlag, New York, 1988).
  5. M. Iansiti, Q. Hu, R. M. Westervelt, and M. Tinkham, Phys. Rev. Lett. 55, 746 (1985); E. G. Gwinn and R. M. Westervelt, Phys. Rev. A 33, 4143 (1986).
  6. C. Grebogi, E. Ott, and J. A. Yorke, Phys. Rev. Lett. 56, 1011 (1986); Physica D 24, 243 (1986).
  7. B.-S. Park, C. Grebogi, E. Ott, and J. A. Yorke, Phys. Rev. A 40, 1576 (1989).
  8. The relation between the uncertainty exponent and the box-counting dimension, α=ND, was rigorously proven for Axiom-A systems [4]. It was conjectured that the same relation holds for more general dynamical systems [1][2].
  9. J. A. Kennedy and J. A. Yorke, Physica D 51, 213 (1991).
  10. H. E. Nusse and J. A. Yorke, Physica D 90, 242 (1996).
  11. L. Poon, J. Campos, E. Ott, and C. Grebogi, Int. J. Bifurcation Chaos Appl. Sci. Eng. 6, 251 (1996).
  12. T. Zhou, F. Moss, and A. Bulsara, Phys. Rev. A 45, 5394 (1992).
  13. M. Ding and S. Kelso, Int. J. Bifurcation Chaos Appl. Sci. Eng. 4, 553 (1994).
  14. T. Kapitaniak and L. O. Chua, Int. J. Bifurcation Chaos Appl. Sci. Eng. 7, 421 (1997).
  15. A. Witt, U. Feudel, and A. Pikovsky, Physica D 109, 180 (1997).
  16. C. Grebogi, E. Ott, S. Pelikan, and J. A. Yorke, Physica D 13, 261 (1984).
  17. Strange nonchaotic attractors typically occur in quasiperiodically driven dynamical systems. Here the word strange refers to the complicated geometry of the attractor: A strange attractor contains an infinite number of points and it is not a smooth manifold in the phase space. The word chaotic refers to the sensitive dependence on initial conditions: trajectories originating from nearby initial conditions on a chaotic attractor diverge exponentially in time. Strange nonchaotic attractors are therefore geometrically complicated, nonetheless they exhibit no sensitive dependence on initial conditions. Some representative papers are F. J. Romeiras, A. Bondeson, E. Ott, T. M. Antonsen, Jr., and C. Grebogi, Physica D 26, 277 (1987); ibid.U. Feudel, J. Kurths, and A. S. Pikovsky, 88, 176 (1995); Y.-C. Lai, U. Feudel, and C. Grebogi, Phys. Rev. E 54, 6070 (1996).
  18. W. L. Ditto, M. L. Spano, H. T. Savage, S. N. Rauseo, J. F. Heagy, and E. Ott, Phys. Rev. Lett. 65, 533 (1990).
  19. M. Napiórkowski, Phys. Rev. A 33, 4423 (1986).
  20. C. Grebogi, E. J. Kostelich, E. Ott, and J. A. Yorke, Physica D 25, 347 (1987).
  21. Y.-C. Lai and R. L. Winslow, Phys. Rev. Lett. 72, 1640 (1994); Physica D 74, 353 (1994).
  22. J. C. Alexander, J. A. Yorke, Z. You, and I. Kan, Int. J. Bifurcation Chaos Appl. Sci. Eng. 2, 795 (1992).
  23. J. Hocking and G. Young, Topology (Addison-Wesley, Reading, MA, 1961).
  24. C. Grebogi, E. Ott, J. A. Yorke, and H. E. Nusse, Ann. (N.Y.) Acad. Sci. 497, 117 (1987).
  25. See, for example, E. M. Oblow, Phys. Lett. A 128, 406 (1988).
  26. C. Grebogi, E. Ott, and J. A. Yorke, Phys. Rev. Lett. 48, 1507 (1982); Physica D 7, 181 (1983).
  27. C. Mira and T. Narayaninsamy, Int. J. Bifurcation Chaos Appl. Sci. Eng. 3, 187 (1993).
  28. B.-S. Park, C. Grebogi, and Y.-C. Lai, Int. J. Bifurcation Chaos Appl. Sci. Eng. 2, 533 (1992).
  29. R. L. Devaney, An Introduction to Chaotic Dynamical Systems (Benjamin Cummings, Menlo Park, 1986).

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