English

Solyanik estimates in ergodic theory

Classical Analysis and ODEs 2016-12-05 v1 Dynamical Systems

Abstract

Let U1,,UnU_1, \ldots, U_n be a collection of commuting measure preserving transformations on a probability space (Ω,Σ,μ)(\Omega, \Sigma, \mu). Associated with these measure preserving transformations is the ergodic strong maximal operator MS\mathsf M ^\ast _{\mathsf S} given by MSf(ω):=sup0RRn1#(RZn)(j1,,jn)RZnf(U1j1Unjnω), \mathsf M ^\ast _{\mathsf S} f(\omega) := \sup_{0 \in R \subset \mathbb{R}^n}\frac{1}{\#(R \cap \mathbb{Z}^n)}\sum_{(j_1, \ldots, j_n) \in R\cap \mathbb{Z}^n}\big|f(U_1^{j_1}\cdots U_n^{j_n}\omega)\big|, where the supremum is taken over all open rectangles in Rn\mathbb{R}^n containing the origin whose sides are parallel to the coordinate axes. For 0<α<10 < \alpha < 1 we define the sharp Tauberian constant of MS\mathsf M ^\ast _{\mathsf S} with respect to α\alpha by CS(α):=supEΩμ(E)>01μ(E)μ({ωΩ:MSχE(ω)>α}). \mathsf C ^\ast _{\mathsf S} (\alpha) := \sup_{\substack{E \subset \Omega \\ \mu(E) > 0}}\frac{1}{\mu(E)}\mu(\{\omega \in \Omega : \mathsf M ^\ast _{\mathsf S} \chi_E (\omega) > \alpha\}). Motivated by previous work of A. A. Solyanik and the authors regarding Solyanik estimates for the geometric strong maximal operator in harmonic analysis, we show that the Solyanik estimate limα1CS(α)=1 \lim_{\alpha \rightarrow 1}\mathsf C ^\ast _{\mathsf S}(\alpha) = 1 holds, and that in particular we have CS(α)1n(11α)1/n\mathsf C ^\ast _{\mathsf S}(\alpha) - 1 \lesssim_n (1 - \frac{1}{\alpha})^{1/n} provided that α\alpha is sufficiently close to 11. Solyanik estimates for centered and uncentered ergodic Hardy-Littlewood maximal operators associated with U1,,UnU_1, \ldots, U_n are shown to hold as well. Further directions for research in the field of ergodic Solyanik estimates are also discussed.

Keywords

Cite

@article{arxiv.1503.02900,
  title  = {Solyanik estimates in ergodic theory},
  author = {Paul A. Hagelstein and Ioannis Parissis},
  journal= {arXiv preprint arXiv:1503.02900},
  year   = {2016}
}
R2 v1 2026-06-22T08:48:44.683Z