The effects of a long-range electronic potential on a one-dimensional chain
of spinless fermions are investigated by numerical techniques (exact diago
nalization of rings with up to 30 sites complemented by finite size analysi
s) and analytic calculations. Due to a competition between the 2k(F) oscill
ations in the density and the (very slow) log divergence of the long wavele
ngth part of the Coulomb potential, the metallic character of the system is
enhanced at intermediate (and up to quite large) length scales. Despite so
me similarities, we found that this quasimetallic regime is not of the Lutt
inger liquid type, as evidenced by strong deviations from predictions of co
nformal field theory and in agreement with the picture of a (very weakly pi
nned) Wigner crystal. When the strength of the Coulomb interaction is subst
antially increased, we observe a smooth crossover to a strongly localized c
harge density wave.