  We study a one-dimensional version of the Hopfield model with long, but
finite range interactions below the critical temperature. In the thermodynamic
limit we obtain large deviation estimates for the distribution of the ``local''
overlaps, the range of the interaction, $\gamma^{-1}$, being the large
parameter. We show in particular that the local overlaps in a typical Gibbs
configuration are constant and equal to one of the mean-field equilibrium
values on a scale $o(\g^{-2})$. We also give estimates on the size of typical
``jumps''. i.e. the regions where transitions from one equilibrium value to
another take place. Contrary to the situation in the ferromagnetic Kac-model,
the structure of the profiles is found to be governed by the quenched disorder
rather than by entropy.
