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Theoretical and Mathematical Physics

On the existence of superconductivity in the Hubbard model

N. N. Bogolyubov, V. A. Moskalenko

Published Jan 1, 1991• 30 citations
Publisher
DOI
10.1007/bf01018492

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In order to provide a numerical criterion for superconductivity, the ground state energy E0{\mathit{E}}_{0}E0​(\ensuremath{\Phi}) is calculated for the attractive and repulsive Hubbard models on a cylinder geometry threaded by a flux \ensuremath{\Phi}. From the functional form of E0{\mathit{E}}_{0}E0​(\ensuremath{\Phi}), superconducting ground states may be identified without prior knowledge of the pairing symmetry. E0{\mathit{E}}_{0}E0​(\ensuremath{\Phi}) is calculated with Monte Carlo methods. For the attractive Hubbard model, our results confirm the existence of a superconducting ground state. In contrast, our results show that the quarter-filled repulsive Hubbard model is not superconducting and that a Hartree-Fock paramagnetic approximation fits the data very well.
Variational tests are performed for current order parameters as probable sources of the pseudogap normal state of cuprates. The calculations are carried out based on the states with correlations of the valence bond type whose formation can induce in principle both the superconducting order of the d symmetry and current phases. It is shown for the t-t′ -U Hubbard models with a large value of U (∼8 t ) and the Hubbard splitting of the conduction band that (1) phases of alternating charge and longitudinal spin currents cannot be realized and (2) transverse spin currents are not compatible with the superconducting order and they could exist against the normal-state background only within a very narrow doping region near the optimal one. This region does not correspond to the region of existence of a pseudogap in cuprates, which refutes the above-mentioned hypothesis of the pseudogap origin. The requirements to the parameters of models for which the consideration of correlations of the valence bond type yields a reasonable phase curve. The existence of current phases in the t-t′-U-V Hubbard models with a strong interaction ( V >0.25t) of particles in neighboring sites is predicted when the d -superconductivity is completely suppressed.
We consider extended versions of the Hubbard model which contain additional interactions between nearest neighbors. In this Letter we show that a large class of these models has a superconducting ground state in arbitrary dimensions. In some special cases we are able to find the complete phase diagram. The superconducting phase exists even for moderate repulsive values of the Hubbard interaction UUU.