We study the quantum dynamics of interstitials and vacancies in a two-dimensional Wigner crystal (WC) using a semiclassical instanton method that is asymptotically exact at low density, i.e., in the rₛ→∞ limit. The dynamics of these point defects mediates magnetism with much higher-energy scales than the exchange energies of the pure WC. Via exact diagonalization of the derived effective Hamiltonians in the single-defect sectors, we find the dynamical corrections to the defect energies. The resulting expression for the interstitial energy extrapolates to 0 at rₛ=rₘᵢₜ≈70 (at rₛ≈30 for a vacancy), suggestive of a self-doping instability to a partially melted WC for some range of rₛ below rₘᵢₜ. We thus propose a ``metallic electron crystal'' phase of the two-dimensional electron gas at intermediate densities between a low-density insulating WC and a high-density Fermi fluid.
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Kim et al. (2024) studied this question.
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