Static and dynamic properties of crystalline phases of two-dimensional electrons in a strong magnetic field

We study the cohesive energy and elastic properties as well as normal modes of the Wigner and bubble crystals of the two-dimensional electron system in higher Landau levels. Using a simple Hartree-Fock approach, we show that the shear moduli (${c}_{66}$'s) of these electronic crystals show a nonmonotonic behavior as a function of the partial filling factor ${\ensuremath{\nu}}^{*}$ at any given Landau level, with ${c}_{66}$ increasing for small values of ${\ensuremath{\nu}}^{*}$, before reaching a maximum at some intermediate filling factor ${\ensuremath{\nu}}_{m}^{*}$, and monotonically decreasing for ${\ensuremath{\nu}}^{*}g{\ensuremath{\nu}}_{m}^{*}$. We also go beyond previous treatments, and study how the phase diagram and elastic properties of electron solids are changed by the effects of screening by electrons in lower Landau levels, and by a finite thickness of the experimental sample. The implications of these results on microwave resonance experiments are briefly discussed.