Given  $\beta \in (1,2]$, let
$\beta \in (1,2]$, let  $T_{\beta }$ be the
$T_{\beta }$ be the  $\beta $-transformation on the unit circle
$\beta $-transformation on the unit circle  $[0,1)$ such that
$[0,1)$ such that  $T_{\beta }(x)=\beta x\pmod 1$. For each
$T_{\beta }(x)=\beta x\pmod 1$. For each  $t\in [0,1)$, let
$t\in [0,1)$, let  $K_{\beta }(t)$ be the survivor set consisting of all
$K_{\beta }(t)$ be the survivor set consisting of all  $x\in [0,1)$ whose orbit
$x\in [0,1)$ whose orbit  $\{T^{n}_{\beta }(x): n\ge 0\}$ never hits the open interval
$\{T^{n}_{\beta }(x): n\ge 0\}$ never hits the open interval  $(0,t)$. Kalle et al [Ergod. Th. & Dynam. Sys. 40(9) (2020) 2482–2514] proved that the Hausdorff dimension function
$(0,t)$. Kalle et al [Ergod. Th. & Dynam. Sys. 40(9) (2020) 2482–2514] proved that the Hausdorff dimension function  $t\mapsto \dim _{H} K_{\beta }(t)$ is a non-increasing Devil’s staircase. So there exists a critical value
$t\mapsto \dim _{H} K_{\beta }(t)$ is a non-increasing Devil’s staircase. So there exists a critical value  $\tau (\beta )$ such that
$\tau (\beta )$ such that  $\dim _{H} K_{\beta }(t)>0$ if and only if
$\dim _{H} K_{\beta }(t)>0$ if and only if  $t<\tau (\beta )$. In this paper, we determine the critical value
$t<\tau (\beta )$. In this paper, we determine the critical value  $\tau (\beta )$ for all
$\tau (\beta )$ for all  $\beta \in (1,2]$, answering a question of Kalle et al (2020). For example, we find that for the Komornik–Loreti constant
$\beta \in (1,2]$, answering a question of Kalle et al (2020). For example, we find that for the Komornik–Loreti constant  $\beta \approx 1.78723$, we have
$\beta \approx 1.78723$, we have  $\tau (\beta )=(2-\beta )/(\beta -1)$. Furthermore, we show that (i) the function
$\tau (\beta )=(2-\beta )/(\beta -1)$. Furthermore, we show that (i) the function  $\tau : \beta \mapsto \tau (\beta )$ is left continuous on
$\tau : \beta \mapsto \tau (\beta )$ is left continuous on  $(1,2]$ with right-hand limits everywhere, but has countably infinitely many discontinuities; (ii)
$(1,2]$ with right-hand limits everywhere, but has countably infinitely many discontinuities; (ii)  $\tau $ has no downward jumps, with
$\tau $ has no downward jumps, with  $\tau (1+)=0$ and
$\tau (1+)=0$ and  $\tau (2)=1/2$; and (iii) there exists an open set
$\tau (2)=1/2$; and (iii) there exists an open set  $O\subset (1,2]$, whose complement
$O\subset (1,2]$, whose complement  $(1,2]\setminus O$ has zero Hausdorff dimension, such that
$(1,2]\setminus O$ has zero Hausdorff dimension, such that  $\tau $ is real-analytic, convex, and strictly decreasing on each connected component of O. Consequently, the dimension
$\tau $ is real-analytic, convex, and strictly decreasing on each connected component of O. Consequently, the dimension  $\dim _{H} K_{\beta }(t)$ is not jointly continuous in
$\dim _{H} K_{\beta }(t)$ is not jointly continuous in  $\beta $ and t. Our strategy to find the critical value
$\beta $ and t. Our strategy to find the critical value  $\tau (\beta )$ depends on certain substitutions of Farey words and a renormalization scheme from dynamical systems.
$\tau (\beta )$ depends on certain substitutions of Farey words and a renormalization scheme from dynamical systems.