{"title":"到子位移的等变映射,其点具有小的稳定器","authors":"Anton Bernshteyn","doi":"10.3934/jmd.2023001","DOIUrl":null,"url":null,"abstract":"Let $\\Gamma$ be a countably infinite group. Given $k \\in \\mathbb{N}$, we use $\\mathrm{Free}(k^\\Gamma)$ to denote the free part of the Bernoulli shift action of $\\Gamma$ on $k^\\Gamma$. Seward and Tucker-Drob showed that there exists a free subshift $\\mathcal{S} \\subseteq \\mathrm{Free}(2^\\Gamma)$ such that every free Borel action of $\\Gamma$ on a Polish space admits a Borel $\\Gamma$-equivariant map to $\\mathcal{S}$. Here we generalize this result as follows. Let $\\mathcal{S}$ be a subshift of finite type (for example, $\\mathcal{S}$ could be the set of all proper colorings of the Cayley graph of $\\Gamma$ with some finite number of colors). Suppose that $\\pi \\colon \\mathrm{Free}(k^\\Gamma) \\to \\mathcal{S}$ is a continuous $\\Gamma$-equivariant map and let $\\mathrm{Stab}(\\pi)$ be the set of all group elements that fix every point in the image of $\\pi$. Unless $\\pi$ is constant, $\\mathrm{Stab}(\\pi)$ is a finite normal subgroup of $\\Gamma$. We prove that there exists a subshift $\\mathcal{S}' \\subseteq \\mathcal{S}$ such that the stabilizer of every point in $\\mathcal{S}'$ is $\\mathrm{Stab}(\\pi)$ and every free Borel action of $\\Gamma$ on a Polish space admits a Borel $\\Gamma$-equivariant map to $\\mathcal{S}'$. In particular, if the shift action of $\\Gamma$ on the image of $\\pi$ is faithful (i.e., if $\\mathrm{Stab}(\\pi)$ is trivial), then the subshift $\\mathcal{S}'$ is free. As an application of this general result, we deduce that if $F$ is a finite symmetric subset of $\\Gamma \\setminus \\{\\mathbf{1}\\}$ of size $|F| = d \\geq 1$ and $\\mathrm{Col}(F, d + 1) \\subseteq (d+1)^\\Gamma$ is the set of all proper $(d+1)$-colorings of the Cayley graph of $\\Gamma$ corresponding to $F$, then there is a free subshift $\\mathcal{S} \\subseteq \\mathrm{Col}(F, d+1)$ such that every free Borel action of $\\Gamma$ on a Polish space admits a Borel $\\Gamma$-equivariant map to $\\mathcal{S}$.","PeriodicalId":51087,"journal":{"name":"Journal of Modern Dynamics","volume":" ","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2021-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Equivariant maps to subshifts whose points have small stabilizers\",\"authors\":\"Anton Bernshteyn\",\"doi\":\"10.3934/jmd.2023001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Let $\\\\Gamma$ be a countably infinite group. Given $k \\\\in \\\\mathbb{N}$, we use $\\\\mathrm{Free}(k^\\\\Gamma)$ to denote the free part of the Bernoulli shift action of $\\\\Gamma$ on $k^\\\\Gamma$. Seward and Tucker-Drob showed that there exists a free subshift $\\\\mathcal{S} \\\\subseteq \\\\mathrm{Free}(2^\\\\Gamma)$ such that every free Borel action of $\\\\Gamma$ on a Polish space admits a Borel $\\\\Gamma$-equivariant map to $\\\\mathcal{S}$. Here we generalize this result as follows. Let $\\\\mathcal{S}$ be a subshift of finite type (for example, $\\\\mathcal{S}$ could be the set of all proper colorings of the Cayley graph of $\\\\Gamma$ with some finite number of colors). Suppose that $\\\\pi \\\\colon \\\\mathrm{Free}(k^\\\\Gamma) \\\\to \\\\mathcal{S}$ is a continuous $\\\\Gamma$-equivariant map and let $\\\\mathrm{Stab}(\\\\pi)$ be the set of all group elements that fix every point in the image of $\\\\pi$. Unless $\\\\pi$ is constant, $\\\\mathrm{Stab}(\\\\pi)$ is a finite normal subgroup of $\\\\Gamma$. We prove that there exists a subshift $\\\\mathcal{S}' \\\\subseteq \\\\mathcal{S}$ such that the stabilizer of every point in $\\\\mathcal{S}'$ is $\\\\mathrm{Stab}(\\\\pi)$ and every free Borel action of $\\\\Gamma$ on a Polish space admits a Borel $\\\\Gamma$-equivariant map to $\\\\mathcal{S}'$. In particular, if the shift action of $\\\\Gamma$ on the image of $\\\\pi$ is faithful (i.e., if $\\\\mathrm{Stab}(\\\\pi)$ is trivial), then the subshift $\\\\mathcal{S}'$ is free. As an application of this general result, we deduce that if $F$ is a finite symmetric subset of $\\\\Gamma \\\\setminus \\\\{\\\\mathbf{1}\\\\}$ of size $|F| = d \\\\geq 1$ and $\\\\mathrm{Col}(F, d + 1) \\\\subseteq (d+1)^\\\\Gamma$ is the set of all proper $(d+1)$-colorings of the Cayley graph of $\\\\Gamma$ corresponding to $F$, then there is a free subshift $\\\\mathcal{S} \\\\subseteq \\\\mathrm{Col}(F, d+1)$ such that every free Borel action of $\\\\Gamma$ on a Polish space admits a Borel $\\\\Gamma$-equivariant map to $\\\\mathcal{S}$.\",\"PeriodicalId\":51087,\"journal\":{\"name\":\"Journal of Modern Dynamics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":0.7000,\"publicationDate\":\"2021-06-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Modern Dynamics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.3934/jmd.2023001\",\"RegionNum\":1,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Modern Dynamics","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.3934/jmd.2023001","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
Equivariant maps to subshifts whose points have small stabilizers
Let $\Gamma$ be a countably infinite group. Given $k \in \mathbb{N}$, we use $\mathrm{Free}(k^\Gamma)$ to denote the free part of the Bernoulli shift action of $\Gamma$ on $k^\Gamma$. Seward and Tucker-Drob showed that there exists a free subshift $\mathcal{S} \subseteq \mathrm{Free}(2^\Gamma)$ such that every free Borel action of $\Gamma$ on a Polish space admits a Borel $\Gamma$-equivariant map to $\mathcal{S}$. Here we generalize this result as follows. Let $\mathcal{S}$ be a subshift of finite type (for example, $\mathcal{S}$ could be the set of all proper colorings of the Cayley graph of $\Gamma$ with some finite number of colors). Suppose that $\pi \colon \mathrm{Free}(k^\Gamma) \to \mathcal{S}$ is a continuous $\Gamma$-equivariant map and let $\mathrm{Stab}(\pi)$ be the set of all group elements that fix every point in the image of $\pi$. Unless $\pi$ is constant, $\mathrm{Stab}(\pi)$ is a finite normal subgroup of $\Gamma$. We prove that there exists a subshift $\mathcal{S}' \subseteq \mathcal{S}$ such that the stabilizer of every point in $\mathcal{S}'$ is $\mathrm{Stab}(\pi)$ and every free Borel action of $\Gamma$ on a Polish space admits a Borel $\Gamma$-equivariant map to $\mathcal{S}'$. In particular, if the shift action of $\Gamma$ on the image of $\pi$ is faithful (i.e., if $\mathrm{Stab}(\pi)$ is trivial), then the subshift $\mathcal{S}'$ is free. As an application of this general result, we deduce that if $F$ is a finite symmetric subset of $\Gamma \setminus \{\mathbf{1}\}$ of size $|F| = d \geq 1$ and $\mathrm{Col}(F, d + 1) \subseteq (d+1)^\Gamma$ is the set of all proper $(d+1)$-colorings of the Cayley graph of $\Gamma$ corresponding to $F$, then there is a free subshift $\mathcal{S} \subseteq \mathrm{Col}(F, d+1)$ such that every free Borel action of $\Gamma$ on a Polish space admits a Borel $\Gamma$-equivariant map to $\mathcal{S}$.
期刊介绍:
The Journal of Modern Dynamics (JMD) is dedicated to publishing research articles in active and promising areas in the theory of dynamical systems with particular emphasis on the mutual interaction between dynamics and other major areas of mathematical research, including:
Number theory
Symplectic geometry
Differential geometry
Rigidity
Quantum chaos
Teichmüller theory
Geometric group theory
Harmonic analysis on manifolds.
The journal is published by the American Institute of Mathematical Sciences (AIMS) with the support of the Anatole Katok Center for Dynamical Systems and Geometry at the Pennsylvania State University.