Mott-Hubbard metal-insulator transition at non-integer filling
arXiv:cond-mat/0309067 · doi:10.1103/PhysRevB.69.045112
Abstract
Correlated electrons in a binary alloy are investigated within the Hubbard model and dynamical mean--field theory (DMFT). The random energies have a bimodal probability distribution and an energy separation . We solve the DMFT equations by the numerical renormalization group method at zero temperature, and calculate the spectral density as a function of disorder strength and interaction at different fillings. For filling factors or the lower or upper alloy subband is half filled and the system becomes a Mott insulator at strong interactions, with a correlation gap at the Fermi level. At the metal--insulator transition hysteresis is observed. We also analyze the effective theory in the limit and find good agreement between analytical and numerical results for the critical interaction at which the metal--insulator transition occurs.
9 pages, 7 figures
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