We propose a symmetry breaking scheme for QCD with three massless quarks at
high baryon density wherein the color and flavor SU(3)(color)XSU(3)(L)XSU(
3)(R) symmetries are broken down to the diagonal subgroup SU(3)(color+L+R)
by the formation of a condensate of quark Cooper pairs. We discuss general
properties that follow from this hypothesis, including the existence of gap
s for quark and gluon excitations, the existence of Nambu-Goldstone bosons
which are excitations of the diquark condensate, and the existence of a mod
ified electromagnetic gauge interaction which is unbroken and which assigns
integral charge to the elementary excitations. We present mean-field resul
ts for a Hamiltonian in which the interaction between quarks is modeled by
that induced by single-gluon exchange. We find gaps of order 10-100 MeV for
plausible values of the coupling. We discuss the effects of non-zero tempe
rature, non-zero quark masses and instanton-induced interactions on our res
ults. (C) 1999 Elsevier Science B.V.