In our calculations, there is a wide region of interaction strengths $\gamma$ for which partially spin-polarized states occur. In this regime our HF ground states nearly always have non-collinear magnetic order. We show local spin polarization and charge density profiles of typical partially polarized states in Figs. \[local\_pol2\] and \[local\_dens2\]. The origin of the reduced spatially integrated spin polarization is partly due to variation of spin-orientation, but principally due to a reduction in the average value of the of the [*magnitude*]{} of the local spin polarization. This point is illustrated in Fig. 1 (open circles) and may be inferred from Fig. \[local\_pol2\] (a). The reduction in spin-polarization is due to the occurrence of doubly-occupied orbitals, [*i.e.*]{} to disorder induced charge fluctuations which cannot be accurately described in models which include only the spin degree of freedom. The charged excitations of the ground state in this regime are ungapped and involve population of localized quasiparticle states. We also remark that local density profiles at these relatively small $\gamma$ values, illustrated in in Fig. \[local\_dens2\] (a), follow the effective disorder potential smoothed by the form factor for lowest Landau level electrons. Rapid spatial variation components in the white noise model disorder potential 