From the Fermi Liquid towards the Wigner Solid in Two Dimensions
The quantum-classical crossover from the Fermi liquid towards the Wigner solid is numerically revisited, considering small square lattice models where electrons interact via a Coulomb U/r potential. We review a series of exact numerical results obtained in the presence of weak site disorder for fully polarized electrons (spinless fermions) and when the spin degrees of freedom are included. A novel intermediate regime between the Fermi system of weakly interacting localized particles and the correlated Wigner solid is obtained. A detailed analysis of the non disordered case shows that the intermediate ground state is a solid entangled with an excited liquid. For electrons in two dimensions, this raises the question of the existence of an unnoticed intermediate liquid-solid phase. Using the Coulomb energy to kinetic energy ratio rs ∝ U ∝ ns −1/2, we discuss certain analogies between the numerical results obtained as a function of U for a few particles and the low temperature behaviors obtained as a function of the carrier density n s in two dimensional electron gases. Notably, the new “exotic state of matter” numerically observed at low energies in small clusters occurs at the same intermediate ratios r s than the unexpected low temperature metallic behavior characterizing dilute electron gases. The finite size effects in the limit of strong disorder are eventually studied in the last section, providing two numerical evidences that the weak coupling Fermi limit is delimited by a second order quantum phase transition when one increases U.