1991
DOI: 10.1103/physrevb.43.5622
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Antiferromagnetism in three-band Hubbard model: Local-ansatz approach

Abstract: The ground state of the three-band Hubbard Hamiltonian for Cu02 planes of high-T, superconductors is investigated. Correlations between holes are included by a local-ansatz approach which starts from the Hartree-Fock approximation and emphasizes the local character of hole correlations. It is found that the hole distribution within Cu02 planes and the region of stability of an antiferromagnetic {AF) ground state are significantly modified by hole correlations. At the filling of one hole per Cu02 unit, and for … Show more

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Cited by 19 publications
(7 citation statements)
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“…Local spin-spin correlation function FCI |S i · S j | FCI (i = 1) (right) of the correlated i-FCIQMC wave function | FCI in the metallic RHF one-particle basis. Like previous studies [37][38][39][40][41][42], we find that the exact i-FCIQMC ground state establishes an antiferromagnetic long-range order across the copper sites, illustrated by the staggered magnetization, (Table I). Again, UHF theory reproduces this closely by separating α and β orbitals on two sublattices while yielding identical band structures for both channels.…”
supporting
confidence: 87%
“…Local spin-spin correlation function FCI |S i · S j | FCI (i = 1) (right) of the correlated i-FCIQMC wave function | FCI in the metallic RHF one-particle basis. Like previous studies [37][38][39][40][41][42], we find that the exact i-FCIQMC ground state establishes an antiferromagnetic long-range order across the copper sites, illustrated by the staggered magnetization, (Table I). Again, UHF theory reproduces this closely by separating α and β orbitals on two sublattices while yielding identical band structures for both channels.…”
supporting
confidence: 87%
“…The doping dependence of hole distribution and the fast disappearence of antiferromagnetic (AF) long-range order under doping 5 - 8 have been studied by means of different approaches, namely, the Hartree-Fock approximation, 9 the local ansatz method, 10 a mean-field approximation that includes the disorder introduced by holes, 11 and mean-field slave-boson techniques. 12 • 13 Also, in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…This approach has been successful in repro acing the quasiparticle (QP) bands in NiO [3] and the weakly dispersive states near the Fermi level (FL) in HTS [4]. The covalent character of the localized 3d9 states [5,6] motivated us to consider an extension of a strongly correlated SFM to a CuO2 plane which implements explicitly the mixed valence (MV) behaviour of the p and d-holes.We consider the four-band model for a CuO2 plane including Cu(3dx2_y2) (x), Cu(3d3z 2_ 1 ) (z), and O(2pσ) orbitals, and assume the weak Cu-O hybridization as compared with the Coulomb repulsion at Cu sites (It,, I <G U). Thus, we have integrated out the transitions to the lower Hubbard band (LHB) (3d8) [2] [which is split into one high-spin ( 3 A2) and two low-spin ( " A2, 1 E1) multiplets], while the upper Hubbard band (UHB) (3d 9 ), described by the projected operators, diσ = diσ(1ni,_ σ ), still hybridizes with 2p holes.…”
mentioning
confidence: 99%
“…This approach has been successful in repro acing the quasiparticle (QP) bands in NiO [3] and the weakly dispersive states near the Fermi level (FL) in HTS [4]. The covalent character of the localized 3d9 states [5,6] motivated us to consider an extension of a strongly correlated SFM to a CuO2 plane which implements explicitly the mixed valence (MV) behaviour of the p and d-holes.…”
mentioning
confidence: 99%