High-Tc cuprates such as La2-xSrxCuO4 and YBa2-xCu3O6+x are considered as a system of the electron and hole polar pseudo-Jahn-Teller CuO4 centers [CuO7-4]JT and [CuO5-4]JT, respectively, or a system of the local bosons moving in a lattice of the hole centers. Ground manifold of the polar centers includes three terms 1A1g (Zhang-Rice singlet), 1Eu, 3Eu with different spin multiplicity, orbital degeneracy and parity that provides an unconventional multi-mode behavior of the cuprates. The spin subsystem of the copper oxides within the polar Jahn-Teller CuO4 centers model is a two-component spin liquid and corresponds to a singlet-triplet magnet with, in general, multiparametric non-collinear spin configurations. In the framework of a modified ...
We solve the problem of the effect of strong electron correlations on the homogeneous spin susceptib...
The Cu3O4 layer in Sr2Cu3O4Cl2 is a variant of the square CuO2 lattice of the high-temperature super...
We explore for all wavevectors through the Brillouin zone the dynamic spin susceptibility χtotal + ,...
Spin subsystem of the copper oxides within the polar Jahn-Teller centers model corresponds to a sing...
A cross-section for magnetic neutron scattering in high-Tc cuprates is obtained in the framework of ...
The CuO4-cluster based copper oxides are considered as generalized quantum lattice bose-gas or a sys...
One of the most exciting features of the hole centers CuO45- in doped cuprates is an unusually compl...
An important feature of the high-transition-temperature (high-Tc) copper oxide superconductors is th...
Both theoretical considerations and experimental data point to a more complicated nature of the vale...
The magnetism of lamellar copper oxides, which are the parent materials of high temperature supercon...
We develop a minimal non-BCS model for the CuO2 planes with the on-site Hilbert space reduced to onl...
Starting with a minimal model for the CuO2 planes with the on-site Hilbert space reduced to a charge...
The high-T(sub c) oxide compounds discovered recently exhibit a number of interesting physical prope...
The author reports studies of spin-fluctuation-induced superconductivity in the antiferromagneticall...
The author reports studies of spin-fluctuation-induced superconductivity in the antiferromagneticall...
We solve the problem of the effect of strong electron correlations on the homogeneous spin susceptib...
The Cu3O4 layer in Sr2Cu3O4Cl2 is a variant of the square CuO2 lattice of the high-temperature super...
We explore for all wavevectors through the Brillouin zone the dynamic spin susceptibility χtotal + ,...
Spin subsystem of the copper oxides within the polar Jahn-Teller centers model corresponds to a sing...
A cross-section for magnetic neutron scattering in high-Tc cuprates is obtained in the framework of ...
The CuO4-cluster based copper oxides are considered as generalized quantum lattice bose-gas or a sys...
One of the most exciting features of the hole centers CuO45- in doped cuprates is an unusually compl...
An important feature of the high-transition-temperature (high-Tc) copper oxide superconductors is th...
Both theoretical considerations and experimental data point to a more complicated nature of the vale...
The magnetism of lamellar copper oxides, which are the parent materials of high temperature supercon...
We develop a minimal non-BCS model for the CuO2 planes with the on-site Hilbert space reduced to onl...
Starting with a minimal model for the CuO2 planes with the on-site Hilbert space reduced to a charge...
The high-T(sub c) oxide compounds discovered recently exhibit a number of interesting physical prope...
The author reports studies of spin-fluctuation-induced superconductivity in the antiferromagneticall...
The author reports studies of spin-fluctuation-induced superconductivity in the antiferromagneticall...
We solve the problem of the effect of strong electron correlations on the homogeneous spin susceptib...
The Cu3O4 layer in Sr2Cu3O4Cl2 is a variant of the square CuO2 lattice of the high-temperature super...
We explore for all wavevectors through the Brillouin zone the dynamic spin susceptibility χtotal + ,...