English

Bernoulli convolutions -- 2023

Classical Analysis and ODEs 2023-12-05 v6 Dynamical Systems Number Theory

Abstract

Let θ(1,2)\theta\in(1,2), and μθ\mu_{\theta} be the Bernoulli convolution parametrized by θ\theta, that is, the measure corresponding to the distribution of the random variable n=1anθn\sum_{n=1}^{\infty} a_n\theta^{-n}, where the ana_n are i.i.d. with probability of an=0a_n=0 equal to 12\frac12. As is well known, μθ\mu_\theta is either equivalent to the Lebesgue measure on supp(μθ)\text{supp}(\mu_\theta), or singular. Recall that an algebraic integer >1>1 is called Pisot if all its other Galois conjugates are smaller than 1 in modulus. It is known that μθ\mu_\theta is singular with dimμθ<1\dim\mu_\theta<1 if θ\theta is Pisot. An algebraic integer θ\theta greater than 1 is called a Salem number if all its other Galois conjugates are of modulus 1, except θ1\theta^{-1}. I shall prove that (1) dimμθ=1\dim\mu_\theta=1 if θ\theta is an algebraic non-Pisot number. (2) if θ\theta is Salem, then μθ\mu_\theta is equivalent to the Lebesgue measure on supp(μθ)\text{supp}(\mu_\theta), with an unbounded density in Lp(supp(μθ))L^p(\text{supp}(\mu_\theta)) for all p<p<\infty. (3) Define βθ,x,n=#{a1an:an+1such that x=k=1anθk}. \beta_{\theta,x,n}=\#\left\{a_1\dots a_n: \exists a_{n+1}\dots\text{such that\ } x=\sum_{k=1}^{\infty}a_n\theta^{-k}\right\}. Then limnβθ,x,nn=θdimμθ for μθa.e.x. \lim_{n\to\infty}\sqrt[n]{\beta_{\theta,x,n}}=\theta^{\dim\mu_\theta}\text{\ for}\ \mu_\theta-\text{a.e.} x. (4) Put n=1{k=1nakθkak{1,0,1}}={y0(θ)<y1(θ)<}, \bigcup_{n=1}^\infty\left\{\sum_{k=1}^{n}a_k\theta^k\mid a_k\in\{-1,0,1\}\right\}= \{y_0(\theta)<y_1(\theta)<\cdots\}, and (θ)=lim infn(yn+1(θ)yn(θ)). \ell(\theta)=\liminf_{n\to\infty}(y_{n+1}(\theta)-y_n(\theta)). I shall present a short proof of De-Jun Feng's famous theorem which states that (θ)=0\ell(\theta)=0 for all non-Pisot θ\theta.

Keywords

Cite

@article{arxiv.2311.00569,
  title  = {Bernoulli convolutions -- 2023},
  author = {Nikita Sidorov},
  journal= {arXiv preprint arXiv:2311.00569},
  year   = {2023}
}

Comments

6 pages

R2 v1 2026-06-28T13:08:39.246Z