Abstract
We introduce a microscopic model for electron doped manganites that explains the mechanism of the observed transition from -type antiferromagnetic (-AF) to -type antiferromagnetic (-AF) order under increasing doping by double exchange mechanism. The model unravels the crucial role played by orbital degrees of freedom and explains the observed metal-to-insulator transition by a dimensional crossover at the magnetic phase transition. The specific heat and the spin canting angle found for the -AF phase agree with the experimental findings. As a surprising outcome of the theory we find that spin canting is suppressed in the -AF phase, in agreement with the experiment, due to the Fermi surface topology.
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