  We study the electronic state of the doped Mott-Hubbard insulator within
Dynamical Mean Field Theory. The evolution of the finite temperature spectral
functions as a function of doping show large redistributions of spectral weight
in both antiferromagnetic and paramagnetic phases. In particular, a metallic
antiferromagnetic state is obtained with a low frequency Slater-splitted
quasiparticle peak coexisting with Hubbard bands. In the high temperature
paramagnetic metallic phase, upon reducing doping, the system has a crossover
through a ``bad metal'' state characterized by an anomalous shift of the
quasiparticle peak away from the Fermi energy. We find that the {\it charge}
compressibility of the antiferromagnetic metal is dramatically enhanced upon
approaching the second order N\'eel line.
