We generalize some notions that have played an important
role in dynamics, namely invariant manifolds, to the
more general context of difference equations. In particular,
we study Lagrangian systems in discrete time. We define
invariant manifolds, even if the corresponding difference
equations can not be transformed in a dynamical system.
The results apply to several examples in the Physics literature:
the Frenkel-Kontorova model with long-range interactions
and the Heisenberg model of spin chains with a
perturbation. We use a modification of the parametrization
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