Abstract
We discuss Liouville's theorem for nonsmooth integrable systems of the billiard type and give a scheme of calculation of angle-action variables for the flow. We also deal with the problem of pseudointegrability. We discuss the relationship between the continuous-time (flow) and the discrete-time (map) approaches. We treat all these aspects through a specific billiard—a wedge embedded in a two-dimensional isotropic harmonic potential. Varying the parameters provides two integrable and two pseudointegrable cases. It turns out that the dynamics of one of the latter is indeed integrable in a certain sense. We also address the problem of applying perturbation theory.
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Dagaeff, T. Integrability and pseudointegrability in billiards illustrated by the harmonic wedge. J Stat Phys 83, 39–70 (1996). https://doi.org/10.1007/BF02183639
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DOI: https://doi.org/10.1007/BF02183639