  We show that a non-Fermi liquid state of interacting electrons in two
dimensions is stable in the presence of disorder and is a perfect conductor,
provided the interactions are sufficiently strong. Otherwise, the disorder
leads to localization as in the case of non-interacting electrons. This
conclusion is established by examining the replica field theory in the weak
disorder limit, but in the presence of arbitrary electron-electron interaction.
Thus, a disordered two-dimensional metal is a perfect metal, but not a Fermi
liquid.
