The electron gas with a strong pairing interaction: Three particle correlations and the Thouless instability
arXiv:cond-mat/0009262 · doi:10.1103/PhysRevB.64.144519
Abstract
We derive simplified Faddeev type equations for the three particle T-matrix which are valid in the Hubbard model where only electrons with opposite spins interact. Using the approximation of dynamical mean field theory these equations are partially solved numerically for the attractive Hubbard model. It is shown that the three particle T-matrix contains a term vanishing at the Thouless (or BCS) instability where the two-particle T-matrix diverges. Based on the three particle term we further derive the low density - strong coupling extension for the two-particle vertex function. We therefore understand our equations as a step towards a systematic low density expansion from the weak coupling BCS theory towards the stronger coupling limit.
14 pages, 9 figures
References in corpus (6)
- Four-particle condensate in strongly coupled fermion systems
- Pairing Fluctuation Theory of Superconducting Properties in Underdoped to Overdoped Cuprates
- On the correct strong-coupling limit in the evolution from BCS superconductivity to Bose-Einstein condensation
- A reliable Pade analytical continuation method based on a high accuracy symbolic computation algorithm
- Density-Induced Breaking of Pairs in the Attractive Hubbard Model
- Three-body properties in hot and dense nuclear matter