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Pseudogaps in Strongly Correlated Metals: A generalized dynamical mean-field theory approach | M.V.Sadovskii
; I.A.Nekrasov
; E.Z.Kuchinskii
; Th.Pruschke
; V.I.Anisimov
; | Date: |
24 Aug 2005 | Journal: | Phys. Rev. B 72, 155105 (2005) | Subject: | Strongly Correlated Electrons | cond-mat.str-el | Abstract: | We generalize the dynamical-mean field (DMFT) approximation by including into the DMFT equations some length scale via a momentum dependent ``external’’ self-energy S(k). This external self-energy describes non-local dynamical correlations induced by short-ranged collective SDW-like antiferromagnetic spin (or CDW-like charge) fluctuations. At high enough temperatures these fluctuations can be viewed as a quenched Gaussian random field with finite correlation length. This generalized DMFT+Sk approach is used for the numerical solution of the weakly doped one-band Hubbard model with repulsive Coulomb interaction on a square lattice with nearest and next nearest neighbour hopping. The effective single impurity problem in this generalized DMFT+Sk is solved by numerical renormalization group (NRG). Both types of strongly correlated metals, namely (i) doped Mott insulator and (ii) the case of bandwidth W~U (U - value of local Coulomb interaction) are considered. Densities of states, spectral functions and ARPES spectra calculated within DMFT+Sk show a pseudogap formation near the Fermi level of the quasiparticle band. | Source: | arXiv, cond-mat/0508585 | Services: | Forum | Review | PDF | Favorites |
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