Abstract
We consider autonomous holonomic dynamical systems defined by equations of the form , where are the coefficients of a symmetric (possibly non-metrical) connection and are the generalized forces. We prove a theorem which for these systems determines autonomous and time-dependent first integrals (FIs) of any order in a systematic way, using the `symmetries' of the geometry defined by the dynamical equations. We demonstrate the application of the theorem to compute linear, quadratic, and cubic FIs of various Riemannian and non-Riemannian dynamical systems.
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