Abstract
The phase diagram of correlated, disordered electron systems is calculated within dynamical mean-field theory using the geometrically averaged (”typical”) local density of states. Correlated metal, Mott insulator, and Anderson insulator phases, as well as coexistence and crossover regimes, are identified. The Mott and Anderson insulators are found to be continuously connected.
- Received 31 March 2004
DOI:https://doi.org/10.1103/PhysRevLett.94.056404
©2005 American Physical Society