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arXiv 1503.06451math.DS
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非自仿射测度的熵公式及其在维尔斯特拉斯型函数中的应用

An entropy formula for a non-self-affine measure with application to Weierstrass-type functions

Atsuya Otani

摘要:

设$ τ: [0,1] \rightarrow [0,1] $是一个具有全分支的分段扩张映射.给定满足$ τ' λ> 1 $的$ λ: [0,1] \rightarrow (0,1) $和$ g : [0,1] \rightarrow \mathbb{R} $,研究Weierstrass型函数\[ \sum _{n=0} ^\infty λ^n (x) \, g (τ^n (x)), \],其中$ λ^n (x) := λ(x) λ(τ(x)) \cdots λ(τ^{n-1} (x)) $ .在一定条件下,Bedford证明了它的图的盒数维数是拓扑压力函数\[ s \mapsto P ((1-s) \log τ' + \log λ) . \]的唯一零点,并给出了豪斯多夫维数与这个值一致的一个充分条件.我们采用了动力系统理论的方法,最初用于调查特殊情况下,包括经典的维尔斯特拉斯函数。为此,我们证明了一个新的Ledrappier-Young熵公式,这是一个条件版本的Pesin的公式,不可逆的动力系统。我们的公式适用于上述函数图上的所有提升吉布斯测度,这些测度通常不是自仿射的。

英文摘要:

Let $ τ: [0,1] \rightarrow [0,1] $ be a piecewise expanding map with full branches. Given $ λ: [0,1] \rightarrow (0,1) $ and $ g : [0,1] \rightarrow \mathbb{R} $ satisfying $ τ' λ> 1 $, we study the Weierstrass-type function \[ \sum _{n=0} ^\infty λ^n (x) \, g (τ^n (x)), \] where $ λ^n (x) := λ(x) λ(τ(x)) \cdots λ(τ^{n-1} (x)) $. Under certain conditions, Bedford proved that the box counting dimension of its graph is given as the unique zero of the topological pressure function \[ s \mapsto P ((1-s) \log τ' + \log λ) . \] We give a sufficient condition under which the Hausdorff dimension also coincides with this value. We adopt a dynamical system theoretic approach which was originally used to investigate special cases including the classical Weierstrass functions. For this purpose we prove a new Ledrappier-Young entropy formula, which is a conditional version of Pesin's formula, for non-invertible dynamical systems. Our formula holds for all lifted Gibbs measures on the graph of the above function, which are generally not self-affine.

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