Link to this article: http://journals.cambridge.org/abstract_S014338570700096XHow to cite this article: G. POPOV and P. TOPALOV (2008). Discrete analog of the projective equivalence and integrable billiard tables.Abstract. A class of discrete dynamical systems called projectively (or geodesically) equivalent Lagrangian systems is defined. We prove that these systems admit families of integrals. In the case of geodesically equivalent billiard tables, these integrals are pairwise commuting. We describe a family of geodesically equivalent billiard tables on surfaces of constant curvature. This is a special case of the so-called 'Liouville billiard tables'.
IntroductionThis is part of a series of papers [10][11][12] concerned with the integrability and spectral rigidity of compact Liouville billiard tables of dimensions n ≥ 2. In this paper we define a class of discrete systems whose integrability follows from a simple construction that we call the geodesic equivalence principle. The main idea is that if the equations describing a discrete dynamical system with a configuration space V m of dimension m can be derived via the variational principle from two different Lagrangians, which means that there exist two Lagrangians L andL (L = c 1 L + c 2 , c 1,2 = const) leading to the same discrete motion on V m , then the discrete system admits a family of conservation laws (integrals) on the phase space V m × V m . Our construction is a discrete analog of the projective (or geodesic equivalence) that appears in Riemannian geometry and goes back to the classical works of Painlevé and Levi-Civita. Following Levi-Civita, recall that two Riemannian metrics g andḡ = const · g on a given smooth manifold M n are geodesically equivalent † if and only if they have the same geodesics on M n (up to a parametrization). It was proved in [7,14,15] (see also the references therein) that projective equivalence implies complete integrability of the geodesic flows of g andḡ. As geodesics of a Riemannian metric g are stationary points of the action functional L g [γ ] :=