Mott-Hubbard and Anderson metal-insulator transitions in correlated lattice fermions with binary disorder
arXiv:0911.0934 · doi:10.1103/PhysRevB.81.115111
Abstract
Strongly correlated fermions in a crystal or in an optical lattice in the presence of binary alloy disorder are investigated. We employ the statistical dynamical mean-field theory, which incorporates both, local fluctuations due to disorder and local correlations due to interaction, to solve the Anderson-Hubbard model. Localization due to disorder is studied by means of the probability distribution function of the local density of states. We obtain a complete paramagnetic ground state phase diagram consisting of disordered correlated metal, Anderson-Mott insulator, and band insulator.
10 pages, 11 figures, published version
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