A generalized nu = 2/3 state, which unifies the sharp edge picture of
MacDonald with the soft edge picture of Chang and Beenakker is present
ed and studied in detail. Using an exact relation between correlation
functions of this state and those of the Laughlin nu = 1/3 wave functi
on, the correlation functions of the nu = 2/3 state are determined via
a classical Monte Carlo calculation, for systems up to fifty electron
s. It is found that as a function of the slope of the confining potent
ial there is a sharp transition of the ground state from one descripti
on to the other. The experimental implications are discussed.