CROSSOVER FROM BCS SUPERCONDUCTIVITY TO BOSE-EINSTEIN CONDENSATION - A SELF-CONSISTENT THEORY

A dilute three-dimensional Fermi liquid is considered with an instantaneous attractive short-range interaction. Two sets of self-consistent equations for the temperature dependent fermion Greens function g and the four-point vertex function GAMMA are derived by field theoretic means. The interaction is taken into account using the results of low energy s-wave scattering theory. The crossover region between BCS superconductivity and Bose-Einstein condensation of tightly bound pairs is located near the threshold where in the two-particle scattering problem a virtual or quasi-stationary state turns into a bound state. We show how from our self-consistent equations the BCS theory and the theory of a superfluid Bose gas can be recovered in the weak and strong coupling limit, respectively. In the strong coupling limit we find that there is a repulsive interaction between the composite bosons due to the Pauli exclusion principle. It is described by a positive scattering length a(B) which is twice the scattering length of the fermions, a(B) = 2a(F). Furthermore we find that this interaction reduces the Bose-Einstein transition temperature to leading order by DELTAT(c)/T(c,BE) = - (k(F)a(F))3/3 pi. We show that most of the previous theories of the crossover scenario can be obtained from our theory in mean-field approximation neglecting self consistency.