We consider the effective extended Hubbard Hamiltonian for the cuprates, with nearest-neighbor hopping which depends on the occupation. Using exact diagonalization in a 4 β’ 4 cluster, we obtain a large enhancement of d-wave pairing correlation functions for optimum doping. The physical picture is co
COM framework for d-wave superconductivity in the 2D Hubbard model
β Scribed by Adolfo Avella; Ferdinando Mancini; Evgeny Plekhanov
- Publisher
- Elsevier Science
- Year
- 2010
- Tongue
- English
- Weight
- 256 KB
- Volume
- 470
- Category
- Article
- ISSN
- 0921-4534
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β¦ Synopsis
The two-dimensional Hubbard model has been studied within the Composite Operator Method (COM) [1] starting from a basis made of the two Hubbard composite fields in the Nambu representation and computing the residual self-energy in the non-crossing approximation (NCA) [2]. The charge-charge, spinspin and pair-pair susceptibilities, involved in the calculation of the self-energy within NCA in the paramagnetic phase, has been computed in the two-pole approximation [1]. The analysis of the d-wave superconducting solution additionally requires the calculation of the charge-pair susceptibility. Therefore, we decided to enlarge the bosonic basis and consider a four-component composite bosonic field to be studied within a four-pole approximation. We here report, in some detail, the quite complex calculation framework and the charge-pair susceptibility in the one-loop approximation.
π SIMILAR VOLUMES
The spin-wave velocity c for the repulsive Hubbard model on a square lattice at half-filling is calculated as the square root of spin stiffness over perpendicular susceptibility using the variational Monte Carlo method with Gutzwiller wave function. For 3 < U/t < 12, c increases by 34--15% compared
We constructed the one-particle spectral functions (diagonal and off-diagonal) which reproduce BCS for weak coupling and which take into account the effect of correlations on superconductivity in the attractive Hubbard model. The diagonal spectral function is composed of three peaks and the off-diag