I review recent work on Fermi systems with attractive interactions of
arbitrary strength. First, I describe the results of a functional inte
gral formulation to study the crossover from cooperative Cooper pairin
g to independent bound state formation and condensation. The inadequac
y of a saddle point approximation with increasing coupling is pointed
out, and the importance of temporal (quantum) fluctuations for normal
state properties at intermediate and strong coupling is emphasized. Ne
xt, results from a quantum Monte-Carlo simulation of the two-dimension
al (2D) attractive Hubbard model are described. The intermediate coupl
ing normal state is found to deviate markedly from a canonical Fermi l
iquid: ''spin-gap'' behavior, with 1/T1T approximately chi(T), is foun
d in a degenerate Fermi system.