13.12.2018 | Yonatan Gutman | Introduction to Rokhlin and sofic entropy theories (II) |
6.12.2018 | Yonatan Gutman | Introduction to Rokhlin and sofic entropy theories (I) |
29.11.2018 | Adam Abrams | A survey of mathematical billiards and related systems |
22.11.2018 | Adam Śpiewak | Maximising Bernoulli measures and dimension gaps for countable branched systems |
15.11.2018 | Adam Abrams | Partitions arising from dynamics of complex continued fractions |
8.11.2018 | Reza Mohammadpour Bejargafsheh | Furstenberg's formula for Lyapunov exponents of linear cocycle (3) |
25.10.2018 | Reza Mohammadpour Bejargafsheh | Furstenberg's formula for Lyapunov exponents of linear cocycle (2) |
18.10.2018 | Artem Dudko | On resurgent approach to dynamics of parabolic germs (2) |
11.10.2018 | Reza Mohammadpour Bejargafsheh | Furstenberg's formula for Lyapunov exponents of linear cocycle (1) |
4.10.2018 | Artem Dudko | On resurgent approach to dynamics of parabolic germs (1) |
It is known since a paper by Kifer, Peres and Weiss that dim(μ) is uniformly bounded away from 1 among all probability measures μ on the unit interval which make the digits of the continued fraction expansion i.i.d random variables. I will present a recent paper Maximising Bernoulli measures and dimension gaps for countable branched systems by Simon Baker and Natalia Jurga, where the authors prove that there exists a measure maximising the dimension in this class. The results are valid for a more general class of countable branched systems.
For real continued fractions, the natural extension of the Gauss map has a global attractor with "finite rectangular structure" owing to the "cycle property" satisfied by each algorithm. In this talk I will present a new property satisfied by a large variety of complex continued fraction algorithms and use it to explore the structure of bijectivity domains for natural extensions of complex Gauss maps. These domains can be given as a finite union of Cartesian products in $\mathbb C\times\mathbb C$, where in one complex coordinate the sets come from explicit manipulation of the algorithm, and in the other coordinate the sets are determined by experimental means.