t-U-W Model of a d_{x^2-y^2} Superconductor in the Proximity of an AF Mott Insulator: Diagrammatic Studies vs. QMC Simulations

Details t-U-W Model of a d_{x^2-y^2} Superconductor in the Proximity of an AF Mott Insulator: Diagrammatic Studies vs. QMC Simulations t-U-W Model of a d_{x^2-y^2} Superconductor in the Proximity of an AF Mott Insulator: Diagrammatic Studies vs. QMC Simulations

2000-04-11

arxiv.org/abs/cond-mat/0004171v3

Phys. Rev. B 62, 12395 (2000)

Physics

Condensed Matter

Superconductivity

final version as appeared in PRB; (c) 2000 The American Physical Society; 24 pages, 14 figures

Scientific paper

10.1103/PhysRevB.62.12395

We examine the competition and relationship between an antiferromagnetic (AF) Mott insulating state and a d_{x^2-y^2} superconducting (SC) state in two dimensions using semi-analytical, i. e. diagrammatic calculations of the t-U-W model. The AF Mott insulator is described by the ground state of the half-filled Hubbard model on a square lattice with on-site Coulomb repulsion U and nearest neighbor single-particle hopping t. To this model, an extra term W is added, which depends upon the square of the single-particle nearest-neighbor hopping. Staying at half-band filling and a constant value of U, it was previously shown with Quantum-Monte-Carlo (QMC) simulations that one can generate a quantum transition as a function of the coupling strength, W, between an AF Mott insulating state and a d_{x^2-y^2} SC state. Here we complement these earlier QMC simulations with physically more transparent diagrammatic calculations. We start with a standard Hartree-Fock (HF) calculation to capture the "high-energy" physics of the t-U-W model. Then, we derive and solve the Bethe-Salpeter equation, i. e. we account for fluctuation effects within the time-dependent HF or generalized RPA scheme. Spin- and charge-susceptibility as well as the effective interaction vertex are calculated and systematically compared with QMC data. Finally, the corresponding BCS gap equation obtained for this effective interaction is solved.

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