Phase diagram, energy scales, and nonlocal correlations in the Anderson lattice model

被引:21
作者
Tanaskovic, D. [1 ]
Haule, K. [2 ]
Kotliar, G. [2 ]
Dobrosavljevic, V. [3 ,4 ]
机构
[1] Univ Belgrade, Inst Phys Belgrade, Comp Sci Lab, Belgrade 11080, Serbia
[2] Rutgers State Univ, Dept Phys & Astron, Piscataway, NJ 08854 USA
[3] Florida State Univ, Dept Phys, Tallahassee, FL 32306 USA
[4] Florida State Univ, Natl High Magnet Field Lab, Tallahassee, FL 32306 USA
来源
PHYSICAL REVIEW B | 2011年 / 84卷 / 11期
基金
美国国家科学基金会;
关键词
HEAVY-FERMION SYSTEMS; MEAN-FIELD THEORY; ELECTRICAL-RESISTIVITY; KONDO-LATTICE; PRESSURE; METALS; SUPERCONDUCTIVITY; CRITICALITY; TRANSITION; LIMIT;
D O I
10.1103/PhysRevB.84.115105
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the Anderson lattice model with one f orbital per lattice site as the simplest model which describes generic features of heavy fermion materials. The resistivity and magnetic susceptibility results obtained within dynamical mean-field theory (DMFT) for a nearly half-filled conduction band show the existence of a single energy scale T* which is similar to the single-ion Kondo temperature T-K(o). To determine the importance of intersite correlations, we have also solved the model within cellular DMFT (CDMFT) with two sites in a unit cell. The antiferromagnetic region on the phase diagram is much narrower than in the single-site solution, having a smaller critical hybridization V-c and Neel temperature T-N. At temperatures above T-N the nonlocal correlations are small, and the DMFT paramagnetic solution is in this case practically exact, which justifies the ab initio local density approximation (LDA) + DMFT approach in theoretical studies of heavy fermions. Strong intersite correlations in the CDMFT solution for T < T-N, however, indicate that they have to be properly treated in order to unravel the physical properties near the quantum critical point.
引用
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页数:10
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