2009
DOI: 10.1140/epjst/e2010-01215-2
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Correlated electrons in the presence of disorder

Abstract: Abstract. Several new aspects of the subtle interplay between electronic correlations and disorder are reviewed. First, the dynamical mean-field theory (DMFT) together with the geometrically averaged ("typical") local density of states is employed to compute the ground state phase diagram of the Anderson-Hubbard model at half-filling. This non-perturbative approach is sensitive to Anderson localization on the one-particle level and hence can detect correlated metallic, Mott insulating and Anderson insulating p… Show more

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Cited by 26 publications
(30 citation statements)
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“…Another way of representing this is ρ typ = exp dV i P (V i ) ln ρ i (ω), where V i represents the bare random potential and P (V i ), the probability distribution followed by these bare site energies. While, ρ typ (0) is critical at the Anderson transition 34,35 , the average density of states (ADoS) given by ρ arith (ω) =…”
Section: Introductionmentioning
confidence: 99%
“…Another way of representing this is ρ typ = exp dV i P (V i ) ln ρ i (ω), where V i represents the bare random potential and P (V i ), the probability distribution followed by these bare site energies. While, ρ typ (0) is critical at the Anderson transition 34,35 , the average density of states (ADoS) given by ρ arith (ω) =…”
Section: Introductionmentioning
confidence: 99%
“…Исследование PM-и AF-фаз показало, что беспо-рядок действительно способствует образованию фазы AF-металла, близкой к точке перехода от PM-металла к AF-диэлектрику, но однозначного ответа в [5] получено не было. Узкая область AF-металла была обнаружена в работе [3] между фазами PM-металла и AF-диэлектрика на магнитной фазовой диаграмме основного состояния в рамках неупорядоченной модели Андерсона−Хаббарда на решетке Бете с бесконечным числом ближайших соседей при половинном заполнении зоны.…”
Section: несоизмеримые спиральные спиновые волны в системах с беспоряunclassified
“…Напомним, что переход от AF-металла к AF-диэлектрику был получен в [3], но на решетке Бете с бесконечным числом соседей и n = 1, в то время как мы проводим исследование на квадратной решетке.…”
Section: рисunclassified
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“…Hence an exact, analytic evaluation of the self-consistent set of equations (92), (93) for the local propagator G σ or the effective propagator G σ (iω n ) is not possible. Exact evaluations are only feasible when there is no coupling between the frequencies.…”
Section: Solution Of the Dmft Self-consistency Equationsmentioning
confidence: 99%