  Current Luttinger liquid edge state theories for filling $\nu=2/3$ predict a
non-universal Hall conductance, in disagreement with experiment. Upon inclusion
of random edge tunnelling we find a phase transition into a new
disordered-dominated edge phase. An exact solution of the random model in this
phase gives a quantized Hall conductance of 2/3 and a neutral mode propagating
upstream. The presence of the neutral mode changes the predicted temperature
dependence for tunnelling through a point contact from $T^{2/\nu -2}$ to $T^2$.
