The phase diagram of half-doped perovskite manganites is studied within the
extended double-exchange model. To demonstrate the role of orbital degrees
of freedom both one- and two-orbital models are examined. A rich phase dia
gram is obtained in the mean-filed theory at zero temperature as a function
of J [antiferromagnetic (AFM) superexchange interaction] and V (intersite
Coulomb repulsion). For the one-orbital model a charge-ordered (CO) state a
ppears at any value of V with different types of magnetic order which chang
es with increasing J from ferromagnetic (F) to AFM ones of the types A, C,
and G. The orbital degeneracy results in appearance of a new CE-type spin o
rder that is favorable due to opening of the "dimerization" gap at the Ferm
i surface. In addition, the CO state appears only for V>V-c for F and CE st
ates while the C-type AFM state disappears and A-type AFM state is observed
only at small values of V as a charge disordered one. The relevance of our
results to the experimental data are discussed.