The Hamiltonian Mean Field (HMF) model describes a system of N fully couple
d particles showing a second-order phase transition as a function of the en
ergy. The dynamics of the model presents interesting features in a small en
ergy region below the critical point. In particular, when the particles are
prepared in a "water bag" initial state, the relaxation to equilibrium is
very slow. In the transient time the system lives in a dynamical quasi-stat
ionary state and exhibits anomalous (enhanced) diffusion and Levy walks. In
this paper we study temperature and velocity distribution of the quasi-sta
tionary state and we show that the lifetime of such a state increases with
N. In particular when the N --> infinity limit is taken before the t --> in
finity limit, the results obtained are different from the expected canonica
l predictions. This scenario seems to confirm a recent conjecture proposed
by Tsallis [C. Tsallis, in: S.R.A. Salinas, C. Tsallis (Eds.), Nonextensive
statistical mechanics and thermodynamics, Braz. J. Phys. 29 (1999) 1 cond-
mat/9903356 and contribution to this conference. (C) 2001 Elsevier Science
Ltd. All rights reserved.