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A dynamical classification for crossed products of fiberwise essentially minimal zero-dimensional dynamical systems

Published online by Cambridge University Press:  11 December 2023

PAUL HERSTEDT*
Affiliation:
Department of Mathematics, Ben Gurion University of the Negev, Beer-Sheva 8410501, Southern District, Israel
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Abstract

We prove that crossed products of fiberwise essentially minimal zero-dimensional dynamical systems, a class that includes systems in which all orbit closures are minimal, have isomorphic K-theory if and only if the dynamical systems are strong orbit equivalent. Under the additional assumption that the dynamical systems have no periodic points, this gives a classification theorem including isomorphism of the associated crossed product $C^*$-algebras as well. We additionally explore the K-theory of such crossed products and the Bratteli diagrams associated to the dynamical systems.

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Type
Original Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0), which permits unrestricted re-use, distribution and reproduction, provided the original article is properly cited.
Copyright
© The Author(s), 2023. Published by Cambridge University Press
Figure 0

Figure 1 An illustration of Definition 2.1. For each base $ X_t $, we divide the base into pieces $ Y_{ t , k } $ that come back to $ X_t $ only after applying $ J_{ t , k } $ iterations of the homeomorphism.

Figure 1

Figure 2 An illustration of Example 2.4(2). Each fiber over $ z \in Z $ is a copy of $ Y $, aside from the fiber at $ \infty \in Z $, which is a singleton (this is pictured as the middle fiber). The picture is meant to depict how the singleton is connected to nearby fibers topologically.

Figure 2

Figure 3 An illustration of Example 4.9(1). This is a Bratteli diagram associated to the shift on the one-point compactification of the integers.

Figure 3

Figure 4 An illustration of Example 4.9(2). This is a Bratteli diagram associated to the fiberwise essentially minimal zero-dimensional system in Example 4.9(2).

Figure 4

Figure 5 A partial ordered Bratteli diagram illustrating an example of a situation that violates conclusion (2) of Proposition 4.11. In this picture, $ v \in V_{ \min } $ since there is a minimal edge with a range of $ w_3' $ and a source of $ v $. However, there is no minimal edge with a source of $ v $ and a range that is a minimal vertex (the possibilities are $ w_1' $ and $ w_2' $).

Figure 5

Figure 6 A partial ordered Bratteli diagram illustrating an example of a situation that violates conclusion (3) of Proposition 4.11. In this picture, $ v \in V_{ \min } $ since there is a minimal edge with a range of $ w_3' $ and a source of $ v $ (also one with a range of $ w_2' $). However, even though $ w_1' $ is in $ R ( v ) $, the minimal edge with a range of $ w_1' $ has a source of $ w_1 $, not $ v $.

Figure 6

Figure 7 A partial ordered Bratteli diagram illustrating an example of a situation that violates conclusion (4) of Proposition 4.11. In this picture, $ v \in V_{ \min } $ since there is a minimal edge with a range of $ w_1' $ and a source of $ v $ (also one with a range of $ w_2' $ and one with a range of $ w_3' $). However, $ w_4' $ is not in $ R ( v ) $, but since $ w_2 $ is in $ ( S \circ R ) ( v ) $, $ w_4' $ is in $ ( R \circ S \circ R ) ( v ) $.