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Journal of Physics Condensed Matter

Superconductivity in the two-dimensional t-J model at low electron density

M. Yu. Kagan, Thomas Maurice Rice

Published May 16, 1994• 62 citations
Publisher

Abstract

The two-dimensional t-J model at low electron densities is unstable against various forms of electron pairing at low enough temperatures. At parameter values J/t<<1, the leading instability, although only at very low temperature, is to p-wave pairing similar to the Hubbard model. At values of J/t>1, an instability against d-wave pairing sets in at a higher temperature as found numerically by Dagotto et al (1993). In addition, at values of J/t>2, which are beyond the threshold for a bound state in the low-electron-density limit, a region of predominantly s-wave pairing is found.

DOI
10.1088/0953-8984/6/20/016

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The two-dimensional t-J model at low electron densities is unstable against various forms of electron pairing at low enough temperatures. At parameter values J/t<<1, the leading instability, although only at very low temperature, is to p-wave pairing similar to the Hubbard model. At values of J/t>1, an instability against d-wave pairing sets in at a higher temperature as found numerically by Dagotto et al (1993). In addition, at values of J/t>2, which are beyond the threshold for a bound state in the low-electron-density limit, a region of predominantly s-wave pairing is found.
The equal-time pairing correlation function of the two-dimensional t-J model on a square lattice is studied using a high-temperature expansion method. The sum of the pairing correlation, its spatial dependence, and the correlation length are obtained as functions of temperature down to T≃0.2tT \simeq 0.2 tT≃0.2t. By comparison of single-particle contributions in the correlation functions, we find an effective attractive interaction between quasi-particles in dx2−y2d_{x^2-y^2}dx2−y2​-wave pairings. It is shown that d-wave correlation grows rapidly at low temperatures for 0.5 < n < 0.9, with n being the electron density. The temperature for this growth is roughly scaled by J/2. This is in sharp contrast to the Hubbard model in a weak or intermediate coupling region, where there is no numerical evidence of superconductivity.
We show that for low and moderate fillings the ground state of the two-dimensional Hubbard model with positive-U and nearest-neighbor hopping is unstable with respect to d-wave pairing with dxy{\mathit{d}}_{\mathit{x}\mathit{y}}dxy​ symmetry of the gap wave function: \ensuremath{\Delta}\ensuremath{\sim}sinkx{\mathit{k}}_{\mathit{x}}kx​sinky{\mathit{k}}_{\mathit{y}}ky​. The inclusion of the next-neighbor hopping may either suppress the pairing or change the symmetry of the superconducting state.
We demonstrate the possibility of triplet p-wave pairing at low electron density a large number of models such as 3D and 2D Fermi-gas models with hard-core repulsion, 3D and 2D Hubbard models, and the Shubin-Vonsovsky model. The critical temperature for p-wave pairing can be considerably higher in the spin-polarized case or even in a two-band situation at low density and can reach experimentally observable values of 1–5 K. We also discuss briefly the d-wave pairing and high-Tc superconductivity with Tc ∼ 100 K which arise in the extended Hubbard model and in the generalized t-J model when close to half-filling.
Numerical and analytical studies of several models of correlated electrons are discussed. Based on exact diagonalization and variational Monte Carlo techniques, we have found indications that the two-dimensional t-J model superconducts near phase separation in the regime of quarter-filling density, in agreement with previous results reported by Dagotto and Riera [Phys. Rev. Lett. 70, 682 (1993)]. At this density the dominant channel is dx2{\mathit{d}}_{\mathit{x}}^{2}dx2​-y2{\mathit{y}}^{2}y2, but a transiton to s-wave superconductivity is observed decreasing the electronic density. In addition, the one-band t-U-V model has also been studied using a mean-field approximation. An interesting region of dx2{\mathit{d}}_{\mathit{x}}^{2}dx2​-y2{\mathit{y}}^{2}y2 superconductivity near phase separation is observed in the phase diagram, and its implications for recent self-consistent studies of d-wave condensates in the context of the high-Tc{\mathit{T}}_{\mathit{c}}Tc​ cuprates are briefly discussed. Finally, the two-band Hubbard model on a chain is also analyzed. Superconducting correlations near phase separation exist in this model, as it occurs in the t-J model. Based on these nontrivial examples it is conjectured that electronic models tend to have superconducting phases in the vicinity of phase separation, and this regime of parameter space should be explored first when a new model for superconductivity is proposed. Reciprocally, if it is established that a model does not phase separate, even in an extended parameter space, then we believe that its chances of presenting a superconducting phase are considerably reduced.