Abstract
A comprehensive definition of the term “integrable” is proving to be elusive. Rather, use of this term invokes a variety of intuitive notions (and not infrequently, some lively debate) corresponding to a belief that integrable systems are in some sense “exactly soluble” and exhibit globally (i.e., for all initial conditions) “regular” solutions. In contrast, the term “nonintegrable” is, generally, taken to imply that a system cannot be “solved exactly” and that its solutions can behave in an “irregular” fashion. Here the notion of irregular behavior corresponds to dynamics that are very sensitive to initial conditions, with neighboring trajectories in the phase space locally diverging on the average at an exponential rate. This characteristic is measured by Lyapunov exponents. A system with at least one positive exponent will display irregular motion. In contrast, regular motion is associated with no positive exponents. Unfortunately, the definition of the Lyapunov exponents involves long time averages, their existence is only guaranteed for a limited set of situations and their values are difficult to compute both analytically and numerically. It is unlikely, therefore, that an algorithm which tests a given system for Lyapunov exponents will be a successful test for integrability.
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Flaschka, H., Newell, A.C., Tabor, M. (1991). Integrability. In: Zakharov, V.E. (eds) What Is Integrability?. Springer Series in Nonlinear Dynamics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-88703-1_3
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