English

Toeplitz flows and their ordered K-theory

Operator Algebras 2017-05-31 v1 Dynamical Systems

Abstract

To a Toeplitz flow (X,T)(X,T) we associate an ordered K0K^0-group, denoted K0(X,T)K^0(X,T), which is order isomorphic to the K0K^0-group of the associated (non-commutative) CC^\ast-crossed product C(X)TZC(X)\rtimes_T \mathbb{Z}. However, K0(X,T)K^0(X,T) can be defined in purely dynamical terms, and it turns out to be a complete invariant for (strong) orbit equivalence. We characterize the K0K^0-groups that arise from Toeplitz flows (X,T)(X,T) as exactly those simple dimension groups (G,G+)(G,G^+) that contain a noncyclic subgroup HH of rank one that intersects G+G^+ nontrivially. Furthermore, the Bratteli diagram realization of (G,G+)(G,G^+) can be chosen to have the ERS-property, i.e. the incidence matrices of the Bratteli diagram have equal row sums. We also prove that for any Choquet simplex KK there exists an uncountable family of pairwise non-orbit equivalent Toeplitz flows (X,T)(X,T) such that the set of TT-invariant probability measures M(X,T)M(X,T) is affinely homeomorphic to KK, where the entropy h(T)h(T) may be prescribed beforehand. Furthermore, the analogous result is true if we substitute strong orbit equivalence for orbit equivalence, but in that case we can actually prescibe both the entropy and the maximal equicontinuous factor of (X,T)(X,T). Finally, we present some interesting concrete examples of dimension groups associated to Toeplitz flows.

Keywords

Cite

@article{arxiv.1404.4771,
  title  = {Toeplitz flows and their ordered K-theory},
  author = {Siri-Malén Høynes},
  journal= {arXiv preprint arXiv:1404.4771},
  year   = {2017}
}

Comments

29 pages

R2 v1 2026-06-22T03:53:41.728Z