中文

在$0$处有洞的$\beta$-变换:一般情形

动力系统 2026-02-18 v3

摘要

给定β>1\beta>1,令TβT_\beta为单位圆[0,1)[0,1)上的β\beta-变换,定义为Tβ(x)=βxβxT_\beta(x)=\beta x-\lfloor \beta x\rfloor。对于每个t[0,1)t\in[0,1),令Kβ(t)K_\beta(t)为幸存集,由所有其轨道{Tβn(x):n0}\{T^n_\beta(x): n\ge 0\}从未进入区间[0,t)[0,t)x[0,1)x\in[0,1)组成。Kalle等人[{\em Ergodic Theory Dynam. Systems} {\bf 40} (2020), no.~9, 2482--2514]考虑了β(1,2]\beta\in(1,2]的情形。他们研究了集值分岔集Eβ:={t[0,1):Kβ(t)Kβ(t) t>t}\mathscr{E}_\beta:=\{t\in[0,1): K_\beta(t')\ne K_\beta(t)~\forall t'>t\},并证明了Hausdorff维数函数tdimHKβ(t)t\mapsto\dim_H K_\beta(t)是一个非增的Devil阶梯。在之前的一篇论文[{\em Ergodic Theory Dynam. Systems} {\bf 43} (2023), no.~6, 1785--1828]中,我们确定了对于所有β(1,2]\beta\in(1,2],临界值τ(β):=min{t>0:ηβ(t)=0}\tau(\beta):=\min\{t>0: \eta_\beta(t)=0\}。本文的目的是将这些结果推广到所有β>1\beta>1。除了计算τ(β)\tau(\beta),我们还证明了(i) 函数τ:βτ(β)\tau: \beta\mapsto\tau(\beta)(1,)(1,\infty)上左连续,处处有右极限,但存在可数无穷多个不连续点;(ii) τ\tau没有向下跳跃;(iii) 存在一个开集O(1,)O\subset(1,\infty),其补集(1,)\O(1,\infty)\backslash O的Hausdorff维数为零,使得τ\tauOO的每个连通分量上是实解析、严格凸且严格递减的。我们还证明了分岔集Eβ\mathscr{E}_\beta的几个拓扑性质。将结果从β(1,2]\beta\in(1,2]推广到所有β>1\beta>1的关键是对Farey词进行适当的推广,这些词用于参数化集合OO的连通分量。上述论文中的一些原始证明得到了简化。

关键词

引用

@article{arxiv.2411.03516,
  title  = {The $\beta$-transformation with a hole at $0$: the general case},
  author = {Pieter Allaart and Derong Kong},
  journal= {arXiv preprint arXiv:2411.03516},
  year   = {2026}
}

备注

A new section was added explaining the connection with the map kx mod 1 with k-1 holes. Several other edits and additions were made. A minor inaccuracy was rectified