We examine the occurrence of Bose-Einstein condensation in both nonrel
ativistic and relativistic systems with no self-interactions in a gene
ral setting. A simple condition for the occurrence of Bose-Einstein co
ndensation can be given if we adopt generalized C-functions to define
the quantum theory. We show that the crucial feature governing Bose-Ei
nstein condensation is the dimension q associated with the continuous
part of the eigenvalue spectrum of the Hamiltonian for nonrelativistic
systems or the spatial part of the Klein-Gordon operator for relativi
stic systems. In either case Bose-Einstein condensation can only occur
if q greater than or equal to 3.