Perturbation theory about generalized self-consistent field solution

被引:0
|
作者
Yang, C [1 ]
Kocharian, AN
Chiang, YL
Chen, LY
机构
[1] Calif State Univ Northridge, Dept Phys & Astron, Northridge, CA 91330 USA
[2] Tamkang Univ, Dept Phys, Tamsui 251, Taiwan
[3] Chinese Culture Univ, Dept Phys, Taipei 111, Taiwan
来源
关键词
Hubbard model; perturbation theory; Bethe-ansatz; mean field; random phase approximation;
D O I
10.1142/S021797920502978X
中图分类号
O59 [应用物理学];
学科分类号
摘要
A new efficient converging perturbation technique valid for arbitrary interaction strength U/t and electron concentration n is applied to study strongly correlated electrons within the repulsive Hubbard model. We test the new perturbation expansion theory in terms of interacting quasi-particles about generalized self-consistent field (GSCF) solution in an entire parameter space. The developed perturbation formalism for strong interaction and large perturbation region differs from the traditional theory on the vicinity of non-interacting electrons by incorporating systematically fluctuations of quasi-particles around self-consistent solution. Performed analytical calculations of the ground state properties in the extreme conditions of one dimensionality provide quite reasonable numerical agreement with the Bethe-ansatz results in the intermediate range of U/t and n. The results are compared with the predictions of traditional perturbation theory.
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页码:2225 / 2249
页数:25
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