Hostname: page-component-74656f9884-2dmjx Total loading time: 0 Render date: 2026-11-07T08:04:41.081Z Has data issue: false hasContentIssue false

Loosely Bernoulli odometer-based systems whose corresponding circular systems are not loosely Bernoulli

Published online by Cambridge University Press:  01 October 2021

MARLIES GERBER*
Affiliation:
Department of Mathematics, Indiana University, Bloomington, IN 47405, USA
PHILIPP KUNDE
Affiliation:
Department of Mathematics, University of Hamburg, Bundesstraße 55, 20146 Hamburg, Germany (e-mail: philipp.kunde@math.uni-hamburg.de)
Rights & Permissions [Opens in a new window]

Abstract

Foreman and Weiss [Measure preserving diffeomorphisms of the torus are unclassifiable. Preprint, 2020, arXiv:1705.04414] obtained an anti-classification result for smooth ergodic diffeomorphisms, up to measure isomorphism, by using a functor $\mathcal {F}$ (see [Foreman and Weiss, From odometers to circular systems: a global structure theorem. J. Mod. Dyn. 15 (2019), 345–423]) mapping odometer-based systems, $\mathcal {OB}$, to circular systems, $\mathcal {CB}$. This functor transfers the classification problem from $\mathcal {OB}$ to $\mathcal {CB}$, and it preserves weakly mixing extensions, compact extensions, factor maps, the rank-one property, and certain types of isomorphisms. Thus it is natural to ask whether $\mathcal {F}$ preserves other dynamical properties. We show that $\mathcal {F}$ does not preserve the loosely Bernoulli property by providing positive and zero-entropy examples of loosely Bernoulli odometer-based systems whose corresponding circular systems are not loosely Bernoulli. We also construct a loosely Bernoulli circular system whose corresponding odometer-based system has zero entropy and is not loosely Bernoulli.

Information

Type
Original Article
Copyright
© The Author(s), 2021. Published by Cambridge University Press
Figure 0

Figure 1 For $j=n,n+1,n+2$, the $\mathcal {Q}_j$ and $\mathcal {R}_j$ are partitions into sets according to the $\mathcal {P}$-names that appear in the indicated j-blocks. The actual numbers of j-blocks are much larger than can be depicted in the figure.

Figure 1

Figure 2 Heuristic representation of two stages of the shifting mechanism. Parts of three $(n+2)$-blocks $\mathtt {B}_1, \mathtt {B}_2, \mathtt {B}_3$ in the odometer-based system and parts of their images $\mathcal {B}_1, \mathcal {B}_2, \mathcal {B}_3$ under the circular operator are represented. The marked letters indicate a best possible $\overline {f}$ match between $\mathcal {B}_1$ and $\mathcal {B}_2$ with a fit of approximately $\big(1-\tfrac 13\big)^2$ (ignoring spacers and boundary effects) while the blocks $\mathtt {B}_1$ and $\mathtt {B}_2$ have a very good fit in the odometer-based system.

Figure 2

Figure 3 Heuristic representation of two stages of the cycling mechanism. Parts of four $(n+2)$-blocks $\mathtt {B}_i$, $i=1,\ldots ,4$, in the odometer-based system and parts of the images $\mathcal {B}_1$ and $\mathcal {B}_2$ under the circular operator (omitting the spacers) are represented. The marked letters indicate a best possible $\overline {f}$ match between $\mathtt {B}_1$ and $\mathtt {B}_2$ with a fit of approximately $\big(1-\tfrac 14\big)^2$ (ignoring boundary effects), while the blocks $\mathcal {B}_1$ and $\mathcal {B}_2$ have a very good fit in the circular system (the lines indicating a best possible $\overline {f}$ match).