The present status of the microscopic foundation of the nuclear Equati
on of State is briefly reviewed. At zero temperature, considerable pro
gress has been done in the last few years in identifying the main phys
ical effects which determine the nuclear saturation curve, at least fo
r not too high densities. Besides the many-body correlations, originat
ing from the bare two-nucleon interactions, three-body forces, meson r
enormalization and non-nucleonic degrees of freedom appear to be of sp
ecial relevance. However, due to the complexity of the problem, a comp
lete solution is still missing. At finite temperature, only very few s
tudies have been presented till now. It is pointed out that the phenom
enology on hot nuclei, obtained in heavy ion collisions, could be used
as a Check for different microscopic theories of the nuclear Equation
of State.