Mott--Hubbard and Anderson Transitions in Dynamical Mean--Field Theory
Krzysztof Byczuk, Walter Hofstetter, and Dieter Vollhardt

TL;DR
This paper investigates the Anderson--Hubbard model at half-filling using dynamical mean-field theory, comparing different averaging schemes to understand the local density of states and phase diagrams at zero temperature.
Contribution
It provides a comparative analysis of geometric and arithmetic averaging schemes within DMFT for the Anderson--Hubbard model, revealing their effects on phase diagrams.
Findings
Differences in local density of states between averaging schemes.
Variation in non-magnetic ground state phase diagrams.
Insights into Mott--Hubbard and Anderson transitions.
Abstract
The Anderson--Hubbard Hamiltonian at half--filling is investigated within dynamical mean--field theory at zero temperature. The local density of states is calculated by taking the geometric and arithmetic mean, respectively. The non--magnetic ground state phase diagrams obtained within the different averaging schemes are compared.
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