Abstract
For hyperbolic systems with singularities, such as dispersing billiards, Pesin theory as developed by Katok and Strelcyn applies to measures that are “adapted” in the sense that they do not give too much weight to neighborhoods of the singularity set. The zero-entropy measures supported on grazing periodic orbits are nonadapted, but it has been an open question whether there are nonadapted measures with positive entropy. We construct such measures for any dispersing billiard with a periodic orbit having a single grazing collision; we then use our construction to show that the thermodynamic formalism for such billiards has a phase transition even when one restricts attention to adapted or to positive entropy measures.
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Notes
See [H, p. 342] for the story of the genesis of this condition, or rather of the slightly stronger condition (a) that appears in [KSLP, P]. The term “adapted” was introduced in [LS], in the context of smooth flows equipped with an invariant measure, as a condition on a Poincaré section (requiring that the boundary \({\mathcal {S}}\) satisfies (1.1) with respect to the induced measure). It has subsequently been used as a condition on measures in systems with singularities [LM, BD1]. For planar dispersing billiards, it is equivalent to assuming the finiteness of the positive Lyapunov exponent almost everywhere (see the proof of Theorem 1.2).
[BD1] constructs a unique measure of maximal entropy under a mild sparse recurrence condition to the singularity set. (If a conjecture of Balint and Toth holds, then this condition is satisfied generically for finite horizon tables [DK].) Yet even without assuming this condition, [BD1] proves that \(P(0) < \infty \). We do not make any assumption of sparse recurrence to singularities in the present paper.
The period 4 is not essential to our construction, yet a second grazing collision along the periodic orbit could complicate the argument and indeed might destroy the horseshoe entirely.
Indeed, since the slopes are \(-{\mathcal {K}}(x_0)\) and \({\mathcal {K}}(x_0)\), respectively, they form an angle equal to 2Arctan\((1/{\mathcal {K}}(x_0))\).
Indeed, a slightly stronger property holds: for every \(x\in R_{k,n,i}\) its local unstable manifold \(W^u(x)\) properly crosses \(R^*\), a proper crossing being a full crossing whose distance from the unstable boundary of \(R^*\) is at least a fixed fraction of the unstable diameter of \(R^*\).
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Acknowledgements
This work started as one of the projects proposed in the workshop Equilibrium states for dynamical systems arising from geometry, held at the American Institute of Mathematics in July 2019. The authors are grateful to AIM for its hospitality. VC was partially supported by NSF Grants DMS-1554794 and DMS-2154378, and by a Simons Foundation Fellowship. MD is partially supported by NSF Grant DMS-2055070. YL was supported by CNPq and Instituto Serrapilheira, Grant “Jangada Dinâmica: Impulsionando Sistemas Dinâmicos na Região Nordeste”. HZ is partially supported by NSF Grant DMS-2220211 and Simons Foundation 706383.
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This work was begun during a workshop held at the American Institute of Mathematics in July 2019. V. Climenhaga was partially supported by National Science Foundation (NSF) Grants DMS-1554794 and DMS-2154378, and by a Simons Foundation Fellowship. M. Demers is partially supported by NSF Grant DMS-2055070. Y. Lima was supported by CNPq and Instituto Serrapilheira, Grant “Jangada Dinâmica: Impulsionando Sistemas Dinâmicos na Região Nordeste”. H.-K. Zhang is partially supported by NSF Grant DMS-2220211 and Simons Foundation Grant 706383.
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Climenhaga, V., Demers, M.F., Lima, Y. et al. Lyapunov Exponents and Nonadapted Measures for Dispersing Billiards. Commun. Math. Phys. 405, 24 (2024). https://doi.org/10.1007/s00220-023-04921-4
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DOI: https://doi.org/10.1007/s00220-023-04921-4