M. Dibari et al., DYNAMICAL BEHAVIOR OF LAGRANGIAN SYSTEMS ON FINSLER MANIFOLDS, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 55(6), 1997, pp. 6448-6458
Tn this paper we develop a theoretical framework devoted to a geometri
cal description of the behavior of dynamical systems and their chaotic
properties. The underground manifold is a Finsler space whose feature
s permit the description of a wide class of dynamical systems such as
those with potentials depending on thr time and velocities for which t
he Riemannian approach is unsuitable. Another appealing feature of thi
s more general setting relies on its very origin: Finsler spaces arise
in a direct way on imposing the invariance for time reparametrization
to a standard variational problem. A Finsler metric is a generalizati
on of the well-known Jacobi and Eisenhart-metrics for conservative dyn
amical systems. We use this geometry to derive the main geometrical in
variants and related expressions that are needed to establish the tran
sition to chaos in very general Lagrangian systems. In order to point
out the versatility and the effectiveness of this extension of the geo
metrical approach, we suggest the introduction of this formalism to so
me interesting dynamical systems for which the Finsler metric is much
more suitable than the Riemannian one. In particular, we present the f
ollowing: (i) an exhaustive description and numerical results for a re
sonant oscillator with a time-dependent potential, (ii) an exact descr
iption (without any approximation) of the dynamics of Bianchi type-IX
cosmological models, and (iii) a geometrical description of the restri
cted three-body problem chose effective potential depends Linearly on
the velocities. In the first case, the numerical integration of the ge
odesics and geodesic deviation equations shows that in the geometrical
picture the source of the exponential instability of trajectories rel
ies on the mechanism of parametric resonance and does not originate fr
om the negativity of curvature.