paper

The complete -spectrum and large deviations for return times for equilibrium states with summable potentials

arXiv:1902.03441

Abstract

Let be a stationary and ergodic process with joint distribution where the random variables take values in a finite set . Let be the first time this process repeats its first symbols of output. It is well-known that converges almost surely to the entropy of the process. Refined properties of (large deviations, multifractality, etc) are encoded in the return-time -spectrum defined as \[ \mathcal{R}(q)=\lim_n\frac{1}{n}\log\int R_n^q \,dμ\quad (q\in\mathbb{R}) \] provided the limit exists. We consider the case where is distributed according to the equilibrium state of a potential with summable variation, and we prove that \[ \mathcal{R}(q) = \begin{cases} P((1-q)φ) & \text{for}\;\; q\geq q_φ^*\\ \sup_η\int φ\, dη& \text{for}\;\; q<q_φ^{*} \end{cases} \] where is the topological pressure of , the supremum is taken over all shift-invariant measures, and is the unique solution of . Unexpectedly, this spectrum does not coincide with the -spectrum of , which is , and does not coincide with the waiting-time -spectrum in general. In fact, the return-time -spectrum coincides with the waiting-time -spectrum if and only if the equilibrium state of is the measure of maximal entropy. As a by-product, we also improve the large deviation asymptotics of .

29 pages, 1 figure, submitted. This is a completely new version. All statements in the previous version are correct, but the proof of the main result relied on a result which turned out to be false. This is now fixed and gave rise to a companion paper by three of the present authors, see arXiv:2101.12381

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