{"title":"双曲流形自连接方向极限集的Hausdorff维数","authors":"Dongryul Kim, Y. Minsky, H. Oh","doi":"10.3934/jmd.2023013","DOIUrl":null,"url":null,"abstract":"The classical result of Patterson and Sullivan says that for a non-elementary convex cocompact subgroup $\\Gamma<\\text{SO}^\\circ (n,1)$, $n\\ge 2$, the Hausdorff dimension of the limit set of $\\Gamma$ is equal to the critical exponent of $\\Gamma$. In this paper, we generalize this result for self-joinings of convex cocompact groups in two ways. Let $\\Delta$ be a finitely generated group and $\\rho_i:\\Delta\\to \\text{SO}^\\circ(n_i,1)$ be a convex cocompact faithful representation of $\\Delta$ for $1\\le i\\le k$. Associated to $\\rho=(\\rho_1, \\cdots, \\rho_k)$, we consider the following self-joining subgroup of $\\prod_{i=1}^k \\text{SO}(n_i,1)$: $$\\Gamma=\\left(\\prod_{i=1}^k\\rho_i\\right)(\\Delta)=\\{(\\rho_1(g), \\cdots, \\rho_k(g)):g\\in \\Delta\\} .$$ (1). Denoting by $\\Lambda\\subset \\prod_{i=1}^k \\mathbb{S}^{n_i-1}$ the limit set of $\\Gamma$, we first prove that $$\\text{dim}_H \\Lambda=\\max_{1\\le i\\le k} \\delta_{\\rho_i}$$ where $\\delta_{\\rho_i}$ is the critical exponent of the subgroup $\\rho_{i}(\\Delta)$. (2). Denoting by $\\Lambda_u\\subset \\Lambda$ the $u$-directional limit set for each $u=(u_1, \\cdots, u_k)$ in the interior of the limit cone of $\\Gamma$, we obtain that for $k\\le 3$, $$ \\frac{\\psi_\\Gamma(u)}{\\max_i u_i }\\le \\text{dim}_H \\Lambda_u \\le \\frac{\\psi_\\Gamma(u)}{\\min_i u_i }$$ where $\\psi_\\Gamma:\\mathbb{R}^k\\to \\mathbb{R}\\cup\\{-\\infty\\}$ is the growth indicator function of $\\Gamma$.","PeriodicalId":51087,"journal":{"name":"Journal of Modern Dynamics","volume":null,"pages":null},"PeriodicalIF":0.7000,"publicationDate":"2023-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"11","resultStr":"{\"title\":\"Hausdorff dimension of directional limit sets for self-joinings of hyperbolic manifolds\",\"authors\":\"Dongryul Kim, Y. Minsky, H. Oh\",\"doi\":\"10.3934/jmd.2023013\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The classical result of Patterson and Sullivan says that for a non-elementary convex cocompact subgroup $\\\\Gamma<\\\\text{SO}^\\\\circ (n,1)$, $n\\\\ge 2$, the Hausdorff dimension of the limit set of $\\\\Gamma$ is equal to the critical exponent of $\\\\Gamma$. In this paper, we generalize this result for self-joinings of convex cocompact groups in two ways. Let $\\\\Delta$ be a finitely generated group and $\\\\rho_i:\\\\Delta\\\\to \\\\text{SO}^\\\\circ(n_i,1)$ be a convex cocompact faithful representation of $\\\\Delta$ for $1\\\\le i\\\\le k$. Associated to $\\\\rho=(\\\\rho_1, \\\\cdots, \\\\rho_k)$, we consider the following self-joining subgroup of $\\\\prod_{i=1}^k \\\\text{SO}(n_i,1)$: $$\\\\Gamma=\\\\left(\\\\prod_{i=1}^k\\\\rho_i\\\\right)(\\\\Delta)=\\\\{(\\\\rho_1(g), \\\\cdots, \\\\rho_k(g)):g\\\\in \\\\Delta\\\\} .$$ (1). Denoting by $\\\\Lambda\\\\subset \\\\prod_{i=1}^k \\\\mathbb{S}^{n_i-1}$ the limit set of $\\\\Gamma$, we first prove that $$\\\\text{dim}_H \\\\Lambda=\\\\max_{1\\\\le i\\\\le k} \\\\delta_{\\\\rho_i}$$ where $\\\\delta_{\\\\rho_i}$ is the critical exponent of the subgroup $\\\\rho_{i}(\\\\Delta)$. (2). Denoting by $\\\\Lambda_u\\\\subset \\\\Lambda$ the $u$-directional limit set for each $u=(u_1, \\\\cdots, u_k)$ in the interior of the limit cone of $\\\\Gamma$, we obtain that for $k\\\\le 3$, $$ \\\\frac{\\\\psi_\\\\Gamma(u)}{\\\\max_i u_i }\\\\le \\\\text{dim}_H \\\\Lambda_u \\\\le \\\\frac{\\\\psi_\\\\Gamma(u)}{\\\\min_i u_i }$$ where $\\\\psi_\\\\Gamma:\\\\mathbb{R}^k\\\\to \\\\mathbb{R}\\\\cup\\\\{-\\\\infty\\\\}$ is the growth indicator function of $\\\\Gamma$.\",\"PeriodicalId\":51087,\"journal\":{\"name\":\"Journal of Modern Dynamics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.7000,\"publicationDate\":\"2023-02-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"11\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Modern Dynamics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.3934/jmd.2023013\",\"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.2023013","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
Hausdorff dimension of directional limit sets for self-joinings of hyperbolic manifolds
The classical result of Patterson and Sullivan says that for a non-elementary convex cocompact subgroup $\Gamma<\text{SO}^\circ (n,1)$, $n\ge 2$, the Hausdorff dimension of the limit set of $\Gamma$ is equal to the critical exponent of $\Gamma$. In this paper, we generalize this result for self-joinings of convex cocompact groups in two ways. Let $\Delta$ be a finitely generated group and $\rho_i:\Delta\to \text{SO}^\circ(n_i,1)$ be a convex cocompact faithful representation of $\Delta$ for $1\le i\le k$. Associated to $\rho=(\rho_1, \cdots, \rho_k)$, we consider the following self-joining subgroup of $\prod_{i=1}^k \text{SO}(n_i,1)$: $$\Gamma=\left(\prod_{i=1}^k\rho_i\right)(\Delta)=\{(\rho_1(g), \cdots, \rho_k(g)):g\in \Delta\} .$$ (1). Denoting by $\Lambda\subset \prod_{i=1}^k \mathbb{S}^{n_i-1}$ the limit set of $\Gamma$, we first prove that $$\text{dim}_H \Lambda=\max_{1\le i\le k} \delta_{\rho_i}$$ where $\delta_{\rho_i}$ is the critical exponent of the subgroup $\rho_{i}(\Delta)$. (2). Denoting by $\Lambda_u\subset \Lambda$ the $u$-directional limit set for each $u=(u_1, \cdots, u_k)$ in the interior of the limit cone of $\Gamma$, we obtain that for $k\le 3$, $$ \frac{\psi_\Gamma(u)}{\max_i u_i }\le \text{dim}_H \Lambda_u \le \frac{\psi_\Gamma(u)}{\min_i u_i }$$ where $\psi_\Gamma:\mathbb{R}^k\to \mathbb{R}\cup\{-\infty\}$ is the growth indicator function of $\Gamma$.
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.