Deryagin, Grigoriev, and Rubakov (DGR) have shown that in finite-density QC
D at infinite N-c the Fermi surface is unstable with respect to the formati
on of chiral waves with wavenumber twice the Fermi momentum, while the BCS
instability is suppressed. We show here that at large, but finite N-c, the
DGR instability only occurs in a finite window of chemical potentials from
above Lambda(QCD) to mu(crit) similar to exp(gamma ln(2)N(c) + O(lnN(c)lnln
N(c)))Lambda(QCD), where gamma approximate to 0.02173. Our analysis shows t
hat, at least in the perturbative regime, the instability occurs only at ex
tremely large N-c, N-c greater than or similar to 1000N(f), where N-f is th
e number of flavors. We conclude that the DGR instability is not likely to
occur in QCD with three colors, where the ground state at finite density is
expected to be a color superconductor. We speculate on the possible struct
ure of the ground state of finite-density QCD with very large N-c. (C) 2000
Elsevier Science B.V. All rights reserved.