Coherence length in superconductors from weak to strong coupling

Abstract

We study the evolution of the superconducting coherence length $ξ_0$ from weak to strong coupling, both within a s-wave and a d-wave lattice model. We show that the identification of $ξ_0$ with the Cooper-pair size $ξ_{pair}$ in the weak-coupling regime is meaningful only for a fully-gapped (e.g., s-wave) superconductor. Instead in the d-wave superconductor, where $ξ_{pair}$ diverges, we show that $ξ_0$ is properly defined as the characteristic length scale for the correlation function of the modulus of the superconducting order parameter. The strong-coupling regime is quite intriguing, since the interplay between particle-particle and particle-hole channel is no more negligible. In the case of s-wave pairing, which allows for an analytical treatment, we show that $ξ_0$ is of order of the lattice spacing at finite densities. In the diluted regime $ξ_0$ diverges, recovering the behavior of the coherence length of a weakly interacting effective bosonic system. Similar results are expected to hold for d-wave superconductors.