John Banks
La Trobe University
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Ergodic Theory and Dynamical Systems | 1997
John Banks
One may often decompose the domain of a topologically transitive map into finitely many regular closed pieces with nowhere dense overlap in such a way that these pieces map into one another in a periodic fashion. We call decompositions of this kind regular periodic decompositions and refer to the number of pieces as the length of the decomposition. If
Journal of Difference Equations and Applications | 2005
John Banks; Belinda Trotta
f
Siam Review | 1994
John Banks; Valentina Dragan
is topologically transitive but
Chaos Solitons & Fractals | 2005
John Banks
f^{n}
Archive | 2003
John Banks; Valentina Dragan; Arthur Jones
is not, then
Discrete and Continuous Dynamical Systems | 1998
John Banks
f
Discrete and Continuous Dynamical Systems | 2013
John Banks; Thi T. D. Nguyen; Piotr Oprocha; Brett Stanley; Belinda Trotta
has a regular periodic decomposition of some length dividing
Discrete and Continuous Dynamical Systems | 2012
John Banks; Brett Stanley
n
Discrete and Continuous Dynamical Systems | 2015
John Banks; Piotr Oprocha; Brett Stanley
. Although a decomposition of a given length is unique, a map may have many decompositions of different lengths. The set of lengths of decompositions of a given map is an ideal in the lattice of natural numbers ordered by divisibility, which we call the decomposition ideal of
Archive | 2003
John Banks; Valentina Dragan; Arthur Jones
f