While both the hole and electron doped cuprates can exhibit dx2-y2-wave superconductivity, the local distribution of the doped carriers is known to be significantly different with the doped holes going primarily on the O sites while the doped electrons go on the Cu sites. Here we report the results of density-matrix-renormalization-group calculations for a three-orbital model of a CuO2 lattice. In addition to the asymmetric dependence of the intra-unit-cell occupation of the Cu and O for hole and electron doping, we find important differences in the longer range spin and charge correlations. As expected, the pair-field response has a dx2-y2-like structure for both the hole and electron doped systems
Recent results regarding electron- and hole-doped CuO2 planes can be rather easily explained by the...
The nature of the effective interaction responsible for pairing in the high-temperature superconduct...
The energy band of oxide superconductors is theoretically investigated when charge and spin fluctuat...
While both the hole and electron doped cuprates can exhibit dx2-y2-wave superconductivity, the local...
We investigate the nature of the electronic ground state and electron-lattice couplings for doped c...
The three-band model relevant to high-temperature copper-oxide superconductors is solved using singl...
In the present paper we study a model which is relevant to an analysis of the effects of the Cu d-d ...
We have considered a two-band Hubbard model having interlaced Cu-3d(x2−y2) and O-2p(x, y) orbitals r...
The local densities of states of an extended Hubbard model describing the Cu02 planes of superconduc...
We have considered a two-band Hubbard model having interlaced Cu-3d(x<SUB>2</SUB>-y<SUB>2</SUB>) and...
Hubbard U is equal to the energy of the insulator to metal transition in Mott insulators. Hubbard U ...
Restricted AccessWe have considered a two-band Hubbard model having interlaced Cu-3d(x2−y2) and O-2p...
We report finite-cluster diagonalizations which clarify the role of apical oxygen orbitals and of th...
Using as a model the Hubbard Hamiltonian, we determine various basic properties of electron-and hole...
Since the discovery of the cuprate high-temperature superconductivity in 1986, a universal phase dia...
Recent results regarding electron- and hole-doped CuO2 planes can be rather easily explained by the...
The nature of the effective interaction responsible for pairing in the high-temperature superconduct...
The energy band of oxide superconductors is theoretically investigated when charge and spin fluctuat...
While both the hole and electron doped cuprates can exhibit dx2-y2-wave superconductivity, the local...
We investigate the nature of the electronic ground state and electron-lattice couplings for doped c...
The three-band model relevant to high-temperature copper-oxide superconductors is solved using singl...
In the present paper we study a model which is relevant to an analysis of the effects of the Cu d-d ...
We have considered a two-band Hubbard model having interlaced Cu-3d(x2−y2) and O-2p(x, y) orbitals r...
The local densities of states of an extended Hubbard model describing the Cu02 planes of superconduc...
We have considered a two-band Hubbard model having interlaced Cu-3d(x<SUB>2</SUB>-y<SUB>2</SUB>) and...
Hubbard U is equal to the energy of the insulator to metal transition in Mott insulators. Hubbard U ...
Restricted AccessWe have considered a two-band Hubbard model having interlaced Cu-3d(x2−y2) and O-2p...
We report finite-cluster diagonalizations which clarify the role of apical oxygen orbitals and of th...
Using as a model the Hubbard Hamiltonian, we determine various basic properties of electron-and hole...
Since the discovery of the cuprate high-temperature superconductivity in 1986, a universal phase dia...
Recent results regarding electron- and hole-doped CuO2 planes can be rather easily explained by the...
The nature of the effective interaction responsible for pairing in the high-temperature superconduct...
The energy band of oxide superconductors is theoretically investigated when charge and spin fluctuat...