Normal phase and superconducting instability in the attractive Hubbard model: a DMFT(NRG) study

被引:15
|
作者
Kuleeva, N. A. [1 ]
Kuchinskii, E. Z. [1 ]
Sadovskii, M. V. [1 ,2 ]
机构
[1] Russian Acad Sci, Inst Electrophys, Ural Branch, Ekaterinburg 620016, Russia
[2] Russian Acad Sci, Inst Met Phys, Ural Branch, Ekaterinburg 620990, Russia
基金
俄罗斯基础研究基金会;
关键词
MEAN-FIELD THEORY; SELF-CONSISTENT THEORY; LOCALIZATION; PHYSICS; WEAK;
D O I
10.1134/S1063776114070036
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We study the normal (nonsuperconducting) phase of the attractive Hubbard model within the dynamical mean field theory (DMFT) using the numerical renormalization group (NRG) as an impurity solver. A wide range of attractive potentials U is considered, from the weak-coupling limit, where superconducting instability is well described by the BCS approximation, to the strong-coupling region, where the superconducting transition is described by Bose condensation of compact Cooper pairs, which are formed at temperatures much exceeding the superconducting transition temperature. We calculate the density of states, the spectral density, and the optical conductivity in the normal phase for this wide range of U, including the disorder effects. We also present the results on superconducting instability of the normal state dependence on the attraction strength U and the degree of disorder. The disorder influence on the critical temperature T (c) is rather weak, suggesting in fact the validity of Anderson's theorem, with the account of the general widening of the conduction band due to disorder.
引用
收藏
页码:264 / 271
页数:8
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