scholarly journals A remark on the Birkhoff ergodic theorem

1971 ◽  
Vol 15 (1) ◽  
pp. 77-79 ◽  
Author(s):  
Donald Ornstein
2017 ◽  
Vol 72 (1-2) ◽  
pp. 715-730
Author(s):  
Nikola Sandrić

2012 ◽  
Vol 47 (3) ◽  
pp. 321-326
Author(s):  
HR Biswas ◽  
MS Islam

In this paper we study one dimensional linear and non-linear maps and its dynamical behavior. We study measure theoretical dynamical behavior of the maps. We study ergodic measure and Birkhoff ergodic theorem. Also, we study some problems using Birkhoff's ergodic theorem. DOI: http://dx.doi.org/10.3329/bjsir.v47i3.13067 Bangladesh J. Sci. Ind. Res. 47(3), 321-326 2012


2019 ◽  
Vol 106 (1-2) ◽  
pp. 52-62
Author(s):  
A. G. Kachurovskii ◽  
I. V. Podvigin

2017 ◽  
Vol 39 (5) ◽  
pp. 1275-1289 ◽  
Author(s):  
AI-HUA FAN

We consider sequences of Davenport type or Gelfond type and prove that sequences of Davenport exponent larger than$\frac{1}{2}$are good sequences of weights for the ergodic theorem, and that the ergodic sums weighted by a sequence of strong Gelfond property are well controlled almost everywhere. We prove that for any$q$-multiplicative sequence, the Gelfond property implies the strong Gelfond property and that sequences realized by dynamical systems can be fully oscillating and have the Gelfond property.


2021 ◽  
Vol 0 (0) ◽  
pp. 0
Author(s):  
Kai Tao

<p style='text-indent:20px;'>In this paper, we first prove the strong Birkhoff Ergodic Theorem for subharmonic functions with the irrational shift on the Torus. Then, we apply it to the analytic quasi-periodic Jacobi cocycles and show that for suitable frequency and coupling number, if the Lyapunov exponent of these cocycles is positive at one point, then it is positive on an interval centered at this point and Hölder continuous in <inline-formula><tex-math id="M1">\begin{document}$ E $\end{document}</tex-math></inline-formula> on this interval. What's more, if the coupling number of the potential is large, then the Lyapunov exponent is always positive for all irrational frequencies and Hölder continuous in <inline-formula><tex-math id="M2">\begin{document}$ E $\end{document}</tex-math></inline-formula> for all finite Liouville frequencies. For the Schrödinger cocycles, a special case of the Jacobi ones, its Lyapunov exponent is also Hölder continuous in the frequency and the lengths of the intervals where the Hölder condition of the Lyapunov exponent holds only depend on the coupling number.</p>


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