KMS states on uniform Roe algebras

Abstract We initiate the treatment of KMS states on uniform Roe algebras $\mathrm {C}^{*}_u(X)$ for a class of naturally occurring flows on these algebras. We show that KMS states on $\mathrm {C}^{*}_u(X)$ always factor through the diagonal operators $\ell_{\infty} (X)$ . We show the study of those states splits into understanding their strongly continuous KMS states and the KMS states which vanish on the ideal of compact operators. We show strongly continuous states are always unique when they exist and we give explicit formulas for them. We link the study of KMS states which vanish on the compacts to the Higson corona of X and provide lower bounds for the cardinality of the set of extreme KMS states. Lastly, we apply our theory to the n -branching tree: in this example, $\beta =\log (n)$ is a phase transition admitting $2^{2^{\aleph _0}}$ KMS states, no KMS states for smaller inverse temperatures, and a unique one for larger ones (the Gibbs state). Moreover, we show that the behavior of the KMS states around $\beta =\log (n)$ is chaotic.

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Publication Details

Journal
Canadian Mathematical Communications
Published
2025-08-15
DOI
https://doi.org/10.4153/s2976859425100003
Primary Topic
Geochemistry and Geologic Mapping
Type
article
Field-Weighted Citation Impact
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article

KMS states on uniform Roe algebras

Canadian Mathematical Communications
Geochemistry and Geologic Mapping
article

KMS states on uniform Roe algebras

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Abstract

Abstract We initiate the treatment of KMS states on uniform Roe algebras $\mathrm {C}^{*}_u(X)$ for a class of naturally occurring flows on these algebras. We show that KMS states on $\mathrm {C}^{*}_u(X)$ always factor through the diagonal operators $\ell_{\infty} (X)$ . We show the study of those states splits into understanding their strongly continuous KMS states and the KMS states which vanish on the ideal of compact operators. We show strongly continuous states are always unique when they exist and we give explicit formulas for them. We link the study of KMS states which vanish on the compacts to the Higson corona of X and provide lower bounds for the cardinality of the set of extreme KMS states. Lastly, we apply our theory to the n -branching tree: in this example, $\beta =\log (n)$ is a phase transition admitting $2^{2^{\aleph _0}}$ KMS states, no KMS states for smaller inverse temperatures, and a unique one for larger ones (the Gibbs state). Moreover, we show that the behavior of the KMS states around $\beta =\log (n)$ is chaotic.

Canadian Mathematical CommunicationsVol. 1
Instituto Nacional de Matemática Pura e Aplicada (BR), Universidade Federal de Santa Catarina (BR)
Openalex Percentile: Top 70%
Geochemistry and Geologic Mapping
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