  A Fluctuation Theorem (FT), both Classical and Quantum, describes the
large-deviations in the approach to equilibrium of an isolated quasi-integrable
system. Two characteristics make it unusual: (i) it concerns the internal
dynamics of an isolated system without external drive, and (ii) unlike the
usual FT, the system size, or the time, need not be small for the relation to
be relevant, provided the system is close to integrability. As an example, in
the Fermi-Pasta-Ulam chain, the relation gives information on the ratio of
probability of death to resurrection of solitons. For a coarse-grained system
the FT describes how the system `skis' down the (minus) entropy landscape:
always descending but generically not along a gradient line.
