Recently, based on the study of long, disordered, one-dimensional chai
ns, it has been proposed that disorder is in the origin of the metalli
c transition in conducting polymers. Disorder could induce the appeara
nce of extended (conducting) states near the Fermi level. It has been
argued that this kind of state could not survive if interactions among
chains are taken into account. In this work we show that the extended
states can survive. even considering the interactions among chains. T
he electronic density of states of long chains were obtained through t
he use of the negative factor counting technique coupled to a tight-bi
nding hamiltonian.