Properties of covariant Lyapunov vectors as continuous vector fields

Abstract: We introduce the concept of ``covariant Lyapunov field'', which assigns all the components of covariant Lyapunov vectors at almost all points of the phase space of a dynamical system. We focus on the case in which these fields are overall continuous and also differentiable along individual trajectories. We show that in ergodic systems such fields can be characterized as the global solutions of a differential equation on the phase space. Due to the arbitrariness in the choice of a multiplicative scalar factor for the Lyapunov vector at each point of the phase space, this differential equation presents a gauge invariance that is formally analogous to that of quantum electrodynamics. Under the hypothesis that the covariant Lyapunov field is overall differentiable, we give a geometric interpretation of our result: each 2-dimensional foliation of the space that contains whole trajectories is univocally associated with a Lyapunov exponent and the corresponding covariant Lyapunov field is one of the generators of the foliation.