4.3 Review

Pseudogap phenomena and superconducting fluctuations in Hubbard model for high-Tc cuprates

Journal

JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN
Volume 70, Issue 6, Pages 1659-1680

Publisher

PHYSICAL SOC JAPAN
DOI: 10.1143/JPSJ.70.1659

Keywords

high-T-c cuprates; Hubbard model; pseudogap; strong coupling superconductivity; superconducting fluctuation; spin fluctuation

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The pseudogap phenomena in High-T-c cuprates are investigated on the basis of the Hubbard model which includes only the on-site repulsive interaction U. We consider the pairing scenario for the pseudogap. The pseudogap arises from the resonance scattering due to the strong super-conducting fluctuations. First, the electronic state and the anti-ferromagnetic spin fluctuations are calculated by using the fluctuation exchange (FLEX) approximation. The T-matrix which is the propagator of the superconducting fluctuations is calculated by extending the Eliashberg equation. The characteristics of the superconducting fluctuations due to the pairing interaction arising from the spin fluctuations are represented in the T-matrix. The self-energy due to the superconducting fluctuations is calculated by the T-matrix approximation. The pseudogap is shown in the single particle properties and the magnetic properties. Moreover, a comprehensive explanation of the doping dependence of the pseudogap is obtained. Furthermore, we apply the theory to the electron-doped cuprates and obtain the consistent results with the recent experiments. Finally, the self-consistent calculation for the spin fluctuations, superconducting fluctuations and the single particle properties is carried out within the FLEX and the self-consistent T-matrix approximations. The relation between the superconducting fluctuations and the spin fluctuations is clarified. The calculated super-conducting critical temperature T-c is remarkably reduced from the results of the mean field (FLEX) calculation. In particular, it is shown that the critical temperature decreases with decreasing doping in the under-doped region with large U.

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