We study QCD-like theories with pseudoreal fermions at finite baryon densit
y. Such theories include two-color QCD with quarks in the fundamental repre
sentation of the color group as well as any-color QCD with quarks in the ad
joint color representation. In all such theories the lightest baryons are d
iquarks, At zero chemical potential mu they are, together with the pseudosc
alar mesons, the Goldstone modes of a spontaneously broken enlarged chiral
symmetry group. Using symmetry principles, we derive the low-energy effecti
ve Lagrangian for these particles. We find that a second order phase transi
tion occurs at a value of mu equal to half the mass of the Goldstone modes.
For values of mu beyond this point the scalar diquarks Bose condense and t
he diquark condensate is nonzero. We calculate the dependence of the chiral
condensate, the diquark condensate, the baryon charge density, and the mas
ses of the diquark and pseudoscalar excitations on mu at finite bare quark
mass and scaler diquark source. The relevance of our results to lattice QCD
calculations and to real three-color QCD at finite baryon density is discu
ssed. (C) 2000 Elsevier Science B.V. All rights reserved.