Correlated electrons in the presence of disorder

被引:21
作者
Byczuk, K. [1 ,2 ]
Hofstetter, W. [3 ]
Yu, U. [4 ]
Vollhardt, D. [2 ]
机构
[1] Univ Warsaw, Inst Theoret Phys, PL-00681 Warsaw, Poland
[2] Univ Augsburg, Inst Phys, Ctr Elect Correlat & Magnetism, D-86135 Augsburg, Germany
[3] Goethe Univ Frankfurt, Inst Theoret Phys, D-60438 Frankfurt, Germany
[4] Gwangju Inst Sci & Technol, Sch Gen Studies, Kwangju 500712, South Korea
关键词
METAL-INSULATOR-TRANSITION; MEAN-FIELD-THEORY; NUMERICAL RENORMALIZATION-GROUP; ANDERSON-HUBBARD MODEL; DIMENSIONS; LOCALIZATION; FERROMAGNETISM; DIFFUSION; FERMIONS; SYSTEMS;
D O I
10.1140/epjst/e2010-01215-2
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
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 phases and can also describe the competition between Anderson localization and antiferromagnetism. Second, we investigate the effect of binary alloy disorder on ferromagnetism in materials with f-electrons described by the periodic Anderson model. A drastic enhancement of the Curie temperature T-c caused by an increase of the local f-moments in the presence of disordered conduction electrons is discovered and explained.
引用
收藏
页码:135 / 151
页数:17
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