Polymer chains with hard-core interaction on a two-dimensional lattice
are modeled by directed random walks. Two models, one with intersecti
ng walks (IW) and another with non-intersecting walks (NIW) are presen
ted, solved and compared. The exact solution of the two models, based
on a representation using Grassmann variables, leads, surprisingly, to
the same analytic expression for the polymer density and identical ph
ase diagrams. There are three different phases as a function of hoppin
g probability and single site monomer occupancy, with a transition fro
m the dense polymer system to a polymer liquid (A) and a transition fr
om the liquid to an empty lattice (B). Within the liquid phase there e
xists a self-dual line with peculiar properties. The derivative of pol
ymer density with respect to the single site monomer occupancy diverge
s at transitions A and B, but is smooth across and along the self-dual
line. The density-density correlation function along the direction x,
perpendicular to the axis of directedness has a power law decay 1/x2
in the entire liquid phase, in both models. The difference between the
two models shows up only in the behavior of the correlation function
along the self-dual line: it decays exponentially in the IW model and
as 1/x4 in the NIW model.