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We study two-dimensional interacting electrons in a weak perpendicularmagnetic field with the filling factor $\nu \gg 1$ and in the presence of aquenched disorder. In the framework of the Hartree-Fock approximation, weobtain the mean-field phase diagram for the partially filled highest Landaulevel. We find that the CDW state can exist if the Landau level broadening$1/2\tau $ does not exceed the critical value $1/2\tau_{c}=0.038\omega_{H}$.Our analysis of weak crystallization corrections to the mean-field resultsshows that these corrections are of the order of $(1/\nu)^{2/3}\ll 1$ andtherefore can be neglected

Mean-field phase diagram of two-dimensional electrons with disorder in a weak magnetic field