We consider the "high-energy" single-particle states of a strongly interact
ing electron liquid. These states should be taken into account whenever the
re are strong incoherent effects produced by interactions. Considering the
presence of these particles which are confined in a thin shell in momentum
space around p = (p) over bar > p(F) as well as "low-energy" quasiparticles
we derive an effective model by integrating out the "high-energy" fields.
The resulting theory produces an effective interaction for the quasiparticl
es which may be large and negative. This produces an instability which driv
es the electron liquid towards superconductivity or another non-perturbativ
e regime.