Fourth-Order Perturbation Expansion for Hubbard Model on a Two-Dimensional Square Lattice

dc.creatorIkeda, H.
dc.creatorShinkai, S.
dc.creatorYamada, K.
dc.date2008-10-10
dc.date.accessioned2026-07-07T10:09:07Z
dc.date.available2026-07-07T10:09:07Z
dc.descriptionWe investigate the Hubbard model on a two-dimensional square lattice by the perturbation expansion to the fourth order in the on-site Coulomb repulsion U. Numerically calculating all diagrams up to the fourth order in self-energy, we examine the convergence of perturbation series in the lattice system. We indicate that the coefficient of each order term rapidly decreases as in the impurity Anderson model for T > 0.1t in the half-filled case, but it holds in the doped case even at lower temperatures. Thus, we can expect that the convergence of perturbation expansion in U is very good in a wide parameter region also in the lattice system, except for T < 0.1t in the half-filled case. We next calculate the density of states in the fourth-order perturbation. In the half-filled case, the shape in a moderate correlation regime is quite different from the three peak structure in the second-order perturbation. Remarkable upper and lower Hubbard bands locate at w = +(-)U/2, and a pseudogap appears at the Fermi level w=0. This is considered as the precursor of the Mott-Hubbard antiferromagnetic structure. In the doped case, quasiparticles with very heavy mass are formed at the Fermi level. Thus, we conclude that the fourth-order perturbation theory overall well explain the asymptotic behaviors in a strong correlation regime.
dc.description17 pages, 20 figures
dc.identifierhttps://arxiv.org/abs/0810.1815
dc.identifierhttp://arxiv.org/abs/0810.1815
dc.identifierJ. Phys. Soc. Jpn. 77, 064707 (2008)
dc.identifierdoi:10.1143/JPSJ.77.064707
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/171223
dc.subjectSuperconductivity
dc.subjectStrongly Correlated Electrons
dc.titleFourth-Order Perturbation Expansion for Hubbard Model on a Two-Dimensional Square Lattice
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