We study the anisotropic magnetic structures exhibited by electron-doped ma
nganites using a model which incorporates the double exchange between orbit
ally degenerate e(g) electrons and the superexchange between t(2g) electron
s with realistic values of the Hund's coupling (J(H)) the superexchange cou
pling (J(AF)) and the bandwidth (W). We look at the relative stabilities of
the G-, C-, and A-type antiferromagnetic phases. In particular we find tha
t the G phase is stable for low electron doping as seen in experiments. We
find good agreement with the experimentally observed magnetic phase diagram
s of electron-doped manganites (x>0.5) such as Nd1-xSrxMnO3, Pr1-xSrxMnO3,
and Sm1-xCaxMnO3. We can also explain the experimentally observed orbital s
tructures of the C and A phases. We also extend our calculation for electro
n-doped bilayer manganites of the form R(2-2x)A(1+2x)Mn(2)O(7) and predict
that the C phase will be absent in these systems due to their reduced dimen
sionality.