SearcharxivSearch

arXiv · 1812.10593

On the Beta Transformation

Abstract

The beta transformation is the iterated map $\beta x\,\mod1$; it generates the base-$\beta$ expansion of a real number x. Every iterated piece-wise monotonic map is topologically conjugate to the beta transformation. For all but a countable subset of $\beta$, the orbits of $x$ are ergodic; yet it is the finite orbits that determine overall behavior. This is a large text; it splits into four parts. The first part provides a review of general concepts and properties associated with the beta shift. The second part examines the spectrum of the Ruelle-Frobenius-Perron operator, and gives explicit expressions for a set of bounded eigenfunctions. These form a discrete spectrum, accumulating on a circle of radius $1/\beta$ in the complex plane. The third part examines the finite and the periodic orbits. These are in one-to-one correspondence with monic integer polynomials. They are "quasi-cyclotomic" and can be counted with Moreau's necklace-counting function; curiously, they do not have any obvious relation to other systems countable by the necklace function. The positive real roots are dense in the reals; they include the Golden and silver ratios, the Pisot numbers, the n-bonacci (tribonacci, tetranacci, etc.) numbers. The beta-polynomials yoke all of these together into a regular structure. An explicit bijection to the rationals is presented. The fourth part of this text examines small perturbations. These introduce Arnold tongues, which inflate the finite orbits, a set of measure zero, to finite size. This text assumes very little mathematical sophistication on the part of the reader, and should be approachable for any enthusiast with minimal or no prior experience in ergodic theory. Most of the development is casual. As a side effect, the introductory sections are perhaps a fair bit longer than strictly needed to present the new results.

Explore related subjects

Keep this discovery

BibTeXRIS

Linas Vepstas. 2018-12-27. On the Beta Transformation. https://doi.org/10.13140/rg.2.2.17132.26248

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Admissible Fourier Lengths, KAM Reducibility, and Spectral Applications

We develop a perturbative KAM reducibility theory for one-frequency $\mathrm{SL}(2,\mathbb{R})$ cocycles based on an admissible Fourier length $\ell$. The regularity relevant to the iteration is measured by positive adapted Fourier width rather than ordinary smoothness in the Euclidean length $|n|$. The same length governs Fourier decay, truncation and resonance scales, and the arithmetic condition controlling the small divisors. This framework contains the classical analytic and Gevrey settings, while non-monotone choices of $\ell$ allow classical nowhere differentiable Weierstrass-type perturbations and continuous perturbations outside every positive H\"older class. As spectral applications, we obtain purely absolutely continuous spectrum for every phase and $1/2$-H\"older continuity of the integrated density of states for the associated quasiperiodic Schr\"odinger operators. The Aubry dual has pure point spectrum for Lebesgue almost every dual phase, with eigenfunctions exponentially localized in the metric induced by $\ell$. We also construct nowhere differentiable quasiperiodic potentials with purely absolutely continuous Cantor spectrum.

math.DS

Dynamics inside the attracting basins of some skew products

Polynomial skew products in $\mathbb{C}^2$ are maps of the form $F(z,w)=(P(z),Q(z,w))$, where $P$ and $Q$ are polynomials. Their local dynamics have been widely investigated. In this paper, we study the global dynamics inside Fatou components of some skew products. We consider all the inverse images in a Fatou component of a given point and use the Kobayashi metric to measure the distance between points. In the cases we consider, there are always arbitrarily large Kobayashi balls in the complement of these inverse sets.

math.DS

Ergodicity of dynamical systems without uniqueness of orbits

Recently, there has been considerable interest in the study of non-deterministic dynamical systems. To analyze the chaotic behavior of such systems from a measure-theoretic viewpoint, it is desirable to consider ergodicity. However, the classical definition of ergodicity involves invariant sets, whose definition is not unique for non-deterministic dynamical systems. Thus, we are led to the question of which invariance yields an interesting definition of ergodicity. Here, we propose a definition based on the strong backward invariance and show that analogs of classical results hold. We also consider implications of the Birkhoff ergodic theorem for systems without uniqueness of orbits.

math.DS