The effects of a long range electronic potential on a one dimensional chain
of spinless fermions are investigated by numerical techniques and analytic
calculations. Due to a competition between the 2k(F) oscillations in the d
ensity and the log divergence of the long wavelength part of the Coulomb po
tential, the metallic character of the system is enhanced at intermediate (
and up to quite large) lengthscales. We found that this quasi-metallic regi
me is not of the Luttinger Liquid type, as evidenced by strong deviations f
rom predictions of conformal field theory and in agreement with the picture
of a (very weakly pinned) Wigner crystal. When the strength of the Coulomb
interaction is substantially increased. we observe a smooth cross-over to
a strongly localized charge density wave.