Feigenbaum function

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In the study of dynamical systems the term Feigenbaum function has been used to describe two different functions introduced by the physicist Mitchell Feigenbaum:

  • the solution to the Feigenbaum-Cvitanović functional equation; and
  • the scaling function that described the covers of the attractor of the logistic map

Contents

[edit] Functional equation

The functional equation arises in the study of one-dimensional maps that, as a function of a parameter, go through a period-doubling cascade. The functional equation is the mathematical expression of the universality of period doubling. The equation is used to specify a function g and a parameter λ by the relation

 g(x) = \frac{1}{\lambda} g( g(\lambda x ) )

with the boundary conditions

  • g(0) = 1,
  • g′(0) = 0, and
  • g′′(0) < 0

[edit] Scaling function

The Feigenbaum scaling function provides a complete description of the attractor of the logistic map at the end of the period-doubling cascade. The attractor is a Cantor set set, and just as the middle-third Cantor set, it can be covered by a finite set of segments, all bigger than a minimal size dn. For a fixed dn the set of segments forms a cover Δn of the attractor. The ratio of segments from two consecutive covers, Δn and Δn+1 can be arranged to approximate a function σ, the Feigenbaum scaling function.

[edit] See also

[edit] References

  • M. Feigenbaum (1979). ""The universal metric properties of non-linear transformations"". Journal of Statistical Physics '19': 669. 
  • Mitchell J. Feigenbaum (1980). ""The transition to aperiodic behavior in turbulent systems"". Communications of Mathematical Physics '77': 65–86. 
  • Mitchell J. Feigenbaum, "Universal Behavior in Nonlinear Systems", Physica 7D (1983) pp 16-39. Bound as Order in Chaos, Proceedings of the International Conference on Order and Chaos held at the Center for Nonlinear Studies, Los Alamos, New Mexico 87545,USA 24-28 May 1982, Eds. David Campbell, Harvey Rose; North-Holland Amsterdam ISBN 0-444-86727-9.