We present results of a Monte Carlo simulation of a (2 + 1)-dimensional Nam
bu-Jona-Lasinio model. In the vacuum phase, the diquark condensate [qq] van
ishes linearly as a function of diquark source j as expected, but simulatio
ns in a region with nonzero baryon density suggest a power-law scaling [qq]
proportional to j(alpha) and hence a critical system for all mu > mu (c).
There is no signal for superfluidity. Comparisons are drawn with the pseudo
gap phase in cuprate superconductors. We also measure the dispersion relati
on E(k) for fermionic excitations, and find results consistent with a sharp
Fermi surface. Any gap Delta is constrained to be much less than the const
ituent quark mass scale Sigma (0).