earlier than in the case at $\nu=1$ ($\gamma\sim1.4-1.6$) because, we believe, a larger number of charged quasiparticles are available to screen the random potential. At this point the system forms what we refer to as a conventional quasiparticle glass (CQG). The conventional Laughlin quasiparticles are initially localized in the deepest minima (or maxima for $\nu<1$) of the effective disorder potential and as the interaction strength increases, or equivalently the depth of the disorder potential wells becomes smaller, the charged quasiparticles rearrange themselves locally into a quasi-triangular Wigner crystal pinned by the strongest of the disorder potential extrema. At larger $\gamma$ we observe a transition from a CQG to a Skyrmion glass. The location of this transition is marked by a reduction of the global polarization from its maximally polarized value. For a specific disorder realization the point of cross over from the CQG to the Skyrmion glass, as illustrated in Fig. \[phase\_diag3\], depends on filling factor and $\tilde g$. The dependence of the transition point on $\tilde{g}$ in this regime can be approximated by considering a simple model for a single Skyrmion trapped at a disorder potential extrema. We approximate its energy by $$E(K)=U(K-K_0)^2+g^*\mu_B B K+\sigma AK\,,
\label{model}$$ where $K$ 