Abstract

In the case of ergodicity much of the structure of a one-dimensional time-discrete dynamical system is already determined by its ordinal structure. We generally discuss this phenomenon by considering the distribution of ordinal patterns, which describe the ups and downs in the orbits of a Borel measurable map on a Borel subset of the real line. On this base, we give a natural ordinal description of the Kolmogorov–Sinai entropy of one-dimensional dynamical systems and relate the Kolmogorov–Sinai entropy to the permutation entropy recently introduced by Bandt and Pompe.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.