  We determine the wave functions for arbitrarily polarized quantum Hall states
by employing the doublet model which has been proposed recently to describe
arbitrarily polarized quantum Hall states. Our findings recover the well known
fully polarized Laughlin wave functions and unpolarized Halperin wave function
for the filling fraction $\nu =2/5$. We have also confirmed by an explicit
One-loop computation that the Hall conductivity does indeed get quantized at
those filling fractions that follow from the model. Finally, we have given a
physical picture for the non-analytic nature of the wave functions, and shown
that quantum fluctuations restore the Kohn mode.
