Deviations from Fermi liquid behavior are well documented in the normal sta
te of the cuprate superconductors, and some of these differences seem to be
related to pretransitional features appearing at temperatures above T-c. T
he observation of a pseudogap, e.g., in ARPES experiments, is a familiar ex
ample of this physics. One potential explanation for this behavior involves
preformed pairs with finite lifetimes existing in the normal state above T
-c. In this way, two characteristic temperatures can be established. A high
er one T* at which pairs begin to form and the actual T-c at which a phase-
coherent superconducting phase is established. In order to test these ideas
we have investigated the negative U Hubbard model in two dimensions in the
fully self-consistent ladder approximation at low electron densities. In t
he nonself-consistent version of this theory the system always shows an ins
tability toward Bose-condensation of infinite lifetime pairs. In contrast t
o this, pairs obtain a finite lifetime due to pair-pair interaction and the
sharp two-particle bound state is strongly lifetime broadened when self-co
nsistency is applied. A quasiparticle scattering rate which varies linearly
with temperature is also found. The fully self-consistent calculation we w
ere able to perform employed a (k) over right arrow-averaged approximation
in which the self-energy loses its (k) over right arrow-dispersion due to a
(k) over right arrow-average. This approximation is found to preserve the
essential physics.