On the Measure of Maximal Entropy for Finite Horizon Sinai Billiard Maps
arXiv:1807.02330 · doi:10.1090/jams/939
Abstract
The Sinai billiard map on the two-torus, i.e., the periodic Lorentz gas, is a discontinuous map. Assuming finite horizon, we propose a definition for the topological entropy of . We prove that is not smaller than the value given by the variational principle, and that it is equal to the definitions of Bowen using spanning or separating sets. Under a mild condition of sparse recurrence to the singularities, we get more: First, using a transfer operator acting on a space of anisotropic distributions, we construct an invariant probability measure of maximal entropy for (i.e., ), we show that has full support and is Bernoulli, and we prove that is the unique measure of maximal entropy, and that it is different from the smooth invariant measure except if all non grazing periodic orbits have multiplier equal to . Second, is equal to the Bowen--Pesin--Pitskel topological entropy of the restriction of to a non-compact domain of continuity. Last, applying results of Lima and Matheus, as upgraded by Buzzi, the map has at least periodic points of period for all large enough .
69 +1 pages, 3 Figures. Version v3 is the electronic copy of the published version. v4 contains a supplement describing minor typos
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