We present the T=0 phase diagram of the double-exchange model (ferromagneti
c Kondo lattice model) for all values of the carrier concentration n and Hu
nd's couplng J, within dynamical mean field theory. We find that depending
on the values of n and J, the ground state is either a ferromagnet, a comme
nsurate antiferromagnet or some other incommensurate phase with intermediat
e wave vectors. The antiferromagnetic phase is separated by first order pha
se boundaries and wide regimes of phase separation. The transition from the
ferromagnetic phase to an incommensurate phase is second order.