Pairing in the Hubbard model: the Cu_{5}O_{4} Cluster versus the Cu-O plane
arXiv:cond-mat/9905272 · doi:10.1007/s100510050129
Abstract
We study the Cu_{5}O_{4} cluster by exact diagonalization of a three-band Hubbard model and show that bound electron or hole pairs are obtained at appropriate fillings, and produce superconducting flux quantisation. The results extend earlier cluster studies and illustrate a canonical transformation approach to pairing that we have developed recently for the full plane. The quasiparticles that in the many-body problem behave like Cooper pairs are W=0 pairs, that is, two-hole eigenstates of the Hubbard Hamiltonian with vanishing on-site repulsion. The cluster allows W=0 pairs of d symmetry, due to a spin fluctuation, and s symmetry, due to a charge fluctuation. Flux quantisation is shown to be a manifestation of symmetry properties that hold for clusters of arbitrary size.
13 pages, 3 figures, a few intermediate steps added for clarity
Cited by in corpus (5)
- W=0 Pairing in Carbon Nanotubes away from Half Filling
- W=0 pairing in Hubbard and related models of low-dimensional superconductors
- Repulsion-Sustained Supercurrent and Flux Quantization in Rings of Symmetric Hubbard Clusters
- Pairing in Cu-O Models: Clues of Joint Electron-Phonon and Electron-Electron Interactions
- "Spin-Disentangled" Exact Diagonalization of Repulsive Hubbard Systems: Superconducting Pair Propagation