Mott-Hubbard transition versus anderson localization in correlated electron systems with disorder

被引：211

作者：

Byczuk, K

Hofstetter, W

Vollhardt, D

机构：

[1] Univ Warsaw, Inst Theoret Phys, PL-00681 Warsaw, Poland

[2] MIT, Condensed Matter Theory Grp, Cambridge, MA 02139 USA

[3] Univ Augsburg, Inst Phys, Ctr Elect Correlat & Magnetism, D-86135 Augsburg, Germany

来源：

PHYSICAL REVIEW LETTERS | 2005年 / 94卷 / 05期

关键词：

D O I：

10.1103/PhysRevLett.94.056404

中图分类号：

O4 [物理学];

学科分类号：

0702 ;

摘要：

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.

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页数：4

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