The Thermodynamic Formalism and the Central Limit Theorem for Stochastic Perturbations of Circle Maps with a Break

A. Dzhalilov, D. Mayer, Abdurahmon Aliyev
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Abstract

Let $T\in C^{2+\varepsilon}(S^{1}\setminus\{x_{b}\})$, $\varepsilon>0$, be an orientation preserving circle homeomorphism with rotation number $\rho_{T}=[k_{1},k_{2},\ldots,k_{m},1,1,\ldots]$, $m\geq 1$, and a single break point $x_{b}$. Stochastic perturbations $\overline{z}_{n+1}=T(\overline{z}_{n})+\sigma\xi_{n+1}$, $\overline{z}_{0}:=z\in S^{1}$ of critical circle maps have been studied some time ago by Diaz-Espinoza and de la Llave, who showed for the resulting sum of random variables a central limit theorem and its rate of convergence. Their approach used the renormalization group technique. We will use here Sinai’s et al. thermodynamic formalism approach, generalised to circle maps with a break point by Dzhalilov et al., to extend the above results to circle homemorphisms with a break point. This and the sequence of dynamical partitions allows us, following earlier work of Vul at al., to establish a symbolic dynamics for any point ${z\in S^{1}}$ and to define a transfer operator whose leading eigenvalue can be used to bound the Lyapunov function. To prove the central limit theorem and its convergence rate we decompose the stochastic sequence via a Taylor expansion in the variables $\xi_{i}$ into the linear term $L_{n}(z_{0})=\xi_{n}+\sum\limits_{k=1}^{n-1}\xi_{k}\prod\limits_{j=k}^{n-1}T^{% \prime}(z_{j})$, ${z_{0}\in S^{1}}$ and a higher order term, which is possible in a neighbourhood $A_{k}^{n}$ of the points $z_{k}$, ${k\leq n-1}$, not containing the break points of $T^{n}$. For this we construct for a certain sequence $\{n_{m}\}$ a series of neighbourhoods $A_{k}^{n_{m}}$ of the points $z_{k}$ which do not contain any break point of the map $T^{q_{n_{m}}}$, $q_{n_{m}}$ the first return times of $T$. The proof of our results follows from the proof of the central limit theorem for the linearized process.
带断裂的圆映射随机扰动的热力学形式和中心极限定理
设$T\in C^{2+\varepsilon}(S^{1}\setminus\{x_{b}\})$, $\varepsilon>0$是一个保持方向的圆同态,旋转数$\rho_{T}=[k_{1},k_{2},\ldots,k_{m},1,1,\ldots]$, $m\geq 1$,有一个断点$x_{b}$。最近Diaz-Espinoza和de la Llave研究了临界圆映射的随机扰动$\overline{z}_{n+1}=T(\overline{z}_{n})+\sigma\xi_{n+1}$, $\overline{z}_{0}:=z\in S^{1}$,他们给出了随机变量和的中心极限定理及其收敛速度。他们的方法使用重整化群技术。在这里,我们将使用西奈等人的热力学形式主义方法(由Dzhalilov等人推广到具有断点的圆映射),将上述结果扩展到具有断点的圆同态。这和动态划分的序列允许我们,在Vul的早期工作之后,建立S^{1}}$中任意点${z\的符号动力学,并定义一个转移算子,其前导特征值可用于约束Lyapunov函数。为了证明中心极限定理及其收敛速度,我们通过变量$\xi_{i}$的泰勒展开式将随机序列分解为线性项$L_{n}(z_{0})=\xi_{n}+\sum\limits_{k=1}^{n-1}\xi_{k}\prod\limits_{j=k}^{n-1}T^{%\素数}(z_{j})$, ${z_{0}\in S^{1}}$和一个高阶项,它可能存在于点$z_{k}$, ${k\leq n-1}$的邻域$A_{k}^{n}$,不包含$T^{n}$的断点。为此,我们为一个特定的序列$\{n_{m}\}$构造了$z_{k}$的一系列邻域$A_{k}^{n_{m}}$,这些邻域$z_{k}$不包含映射$T^{q_{n_{m}} $的断点,$q_{n_{m}}$是$T$的第一次返回次数。从线性化过程的中心极限定理的证明出发,证明了我们的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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