English

The doubling map with asymmetrical holes

Dynamical Systems 2015-07-01 v2

Abstract

Let 0<a<b<10<a<b<1 and let TT be the doubling map. Set J(a,b):={x[0,1]:Tnx(a,b),n0}\mathcal J(a,b):=\{x\in[0,1] : T^nx\notin (a,b), n\ge0\}. In this paper we completely characterize the holes (a,b)(a,b) for which any of the following scenarios holds: {enumerate} J(a,b)\mathcal J(a,b) contains a point x(0,1)x\in(0,1); J(a,b)[\de,1\de]\mathcal J(a,b)\cap [\de,1-\de] is infinite for any fixed \de>0\de>0; J(a,b)\mathcal J(a,b) is uncountable of zero Hausdorff dimension; J(a,b)\mathcal J(a,b) is of positive Hausdorff dimension. {enumerate} In particular, we show that (iv) is always the case if ba<14n=1(122n)0.175092 b-a<\frac14\prod_{n=1}^\infty \bigl(1-2^{-2^n}\bigr)\approx 0.175092 and that this bound is sharp. As a corollary, we give a full description of first and second order critical holes introduced in \cite{SSC} for the doubling map. Furthermore, we show that our model yields a continuum of "routes to chaos" via arbitrary sequences of products of natural numbers, thus generalizing the standard route to chaos via period doubling.

Keywords

Cite

@article{arxiv.1302.2486,
  title  = {The doubling map with asymmetrical holes},
  author = {Paul Glendinning and Nikita Sidorov},
  journal= {arXiv preprint arXiv:1302.2486},
  year   = {2015}
}

Comments

26 pages, 3 figures

R2 v1 2026-06-21T23:24:08.938Z