The phase diagram of strongly interacting matter is explored as a func
tion of temperature and baryon number density. We investigate the poss
ible simultaneous formation of condensates in the conventional quark-a
nti-quark channel (breaking chiral symmetry) and in a quark-quark chan
nel leading to color superconductivity: the spontaneous breaking of co
lor symmetry via the formation of quark Cooper pairs. We point out tha
t for two massless quark flavors a tricritical point in the phase diag
ram separates a chiral symmetry restoring first order transition at hi
gh densities from the second order transition at high temperatures. Aw
ay from the chiral limit this tricritical point becomes a second order
phase transition with Ising model exponents, suggesting that a long c
orrelation length may develop in heavy ion collisions in which the pha
se transition is traversed at the appropriate density.