We calculate the energy of charge-carrier-induced canted ordering in conduc
ting layered antiferromagnetic systems with double exchange. The quantum ap
proach to the d-spins is used. In the jellium model the energy of the cante
d state is lower than the energies of both collinear ferro- and antiferroma
gnetic states over a certain range of charge carrier densities, beginning w
ith arbitrarily small densities. Nevertheless, the canted state cannot be r
ealized, because it is unstable against charge-carrier density fluctuations
. The two-phase ferro-antiferromagnetic state can play the role of an alter
native to canting. The case of an intermediate electronic-impurity phase se
paration is investigated. (C) 1998 American Institute of Physics. [S1063-77
61(98)02612-2].