Negative differential resistance in n-type noncompensated silicon at low temperaturePrischepa, S. L.,
Danilyuk, A. L.,
Trafimenko, A. G.,
Fedotov, A. K.,
Svito, I. A.,
Прищепа, С. Л.,
Данилюк, А. Л. of the NDR. We attribute this effect to the delocalization of the D- states in the
upper Hubbard band due
Negative differential resistance in n-type noncompensated silicon at low temperaturePrischepa, S. L.,
Danilyuk, A. L.,
Trafimenko, A. G.,
Fedotov, A. K.,
Svito, I. A.,
Прищепа, С. Л.,
Данилюк, А. Л. of the NDR. We attribute this effect to the delocalization of the D- states in the
upper Hubbard band due
Dynamic susceptibility in two-dimensional Hubbard model Hubbard and as in the case when chemical potential is displaced in the
upper Hubbard band. It includes
Low temperature conductivity in n-type noncompensated silicon below insulator-metal transitionDanilyuk, A. L.,
Trafimenko, A. G.,
Fedotov, A. K.,
Svito, I. A.,
Prischepa, S. L.,
Данилюк, А. Л.,
Прищепа, С. Л. mechanisms of the conductivity in the presence of two impurity
bands, the
upper and lower
Hubbard bands (UHB
Dynamic susceptibility in two-dimensional Hubbard model Hubbard and as in the case when chemical potential is displaced in the
upper Hubbard band. It includes
Делокализация электронных состояний в n-Si при низких температурахДанилюк, А. Л.,
Трафименко, А. Г.,
Федотов, А. К.,
Прищепа, С. Л.,
Danilyuk, A. L.,
Trafimenko, A. G.,
Fedotov, A. K.,
Prischepa, S. L. with an increase in current can be explained by the exchange of electrons between the
upper Hubbard band, formed
The energy dispersion of the singlet correlated impurity band in layered cuprates cuprates using
Hubbard projection operators. Hund's and Kondo-like exchange, copper-oxygen and oxygen
The spin susceptibility of singlet correlated oxygen band in La2-xSrxCuO4 in terms of two relevant
band models containing the singlet-correlated oxygen
band and the copper character
Charge-excitation picture of Cu NMR Knight shift and relaxation in YBa2Cu4O8 deduced from a 3-band Hubbard model. The starting point is a three-
band Hubbard model comprising a Kondo-like exchange between the copper and oxygen