Cooper pair (CP) binding with both zero and nonzero center-of-mass momenta
(CMM) is studied with a set of renormalized equations assuming a short-rang
ed (attractive) pairwise interfermion interaction. Expanding the associated
dispersion relation in 2D in powers of the CMM, in weak-to-moderate coupli
ng a term linear in the CMM dominates the pair excitation energy, while the
quadratic behavior usually assumed in Bose-Einstein (BE) condensation stud
ies prevails for any coupling only in the limit of zero Fermi velocity when
the Fermi sea disappears, i.e., in vacuum. In 3D this same behavior is obs
erved numerically. The linear term, moreover. exhibits CP breakup beyond a
threshold CMM value which vanishes with coupling. This makes all the excite
d (nonzero-CMM) BE levels with preformed CPs collapse into a single ground
level so that a BCS condensate (where only zero CMM CPs are usually allowed
) appears in zero coupling to be a special case in either 2D or 3D of the B
E condensate of linear-dispersion-relation CPs. (C) 2001 Elsevier Science B
.V. All rights reserved.