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Superlattices and Microstructures

A pairing mechanism in superconductivity due to the screened coulomb field

J. D. Fan, Y. M. Malozovsky

Published Mar 1, 1997• 0 citations
Publisher
DOI
10.1006/spmi.1996.0157

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The occurrence of retarded (with glue) and unretarded (without glue) pairing is thoroughly discussed in cuprates. We analyze some aspects of this problem in the context of the $t\text{\ensuremath{-}}J\text{\ensuremath{-}}V$ model in a large-NNN approximation. When 1/N1/N1/N renormalizations are neglected the mean-field result is recovered, where the unretarded ddd-wave superconducting pairing triggered by the spin-exchange interaction JJJ is obtained. However, the presence of a nonnegligible nearest-neighbors Coulomb interaction V(q)V(\mathbf{q})V(q) kills superconductivity. If the non-double-occupancy constraint and its fluctuations are considered, the situation changes drastically. In this case, V(q)V(\mathbf{q})V(q) is screened making ddd-wave superconductivity very robust. In addition, we show that the early proposal for the presence of an unretarded pairing contribution triggered by the spin-exchange interaction JJJ can be discussed in this context.
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We analyze the effect of the nonvanishing range of electron-electron repulsion on the mechanism of unconventional superconductivity. We present asymptotically exact weak-coupling results for dilute electrons in the continuum and for the 2D extended Hubbard model, as well as density-matrix renormalization group results for the two-leg extended Hubbard model at intermediate couplings, and approximate results for the case of realistically screened Coulomb interactions. We show that Tc{T}_{c}Tc​ is generally suppressed in some pairing channels as longer range interactions increase in strength, but superconductivity is not destroyed. Our results confirm that electron-electron interaction can lead to unconventional superconductivity under physically realistic circumstances.