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The term magnetoelectric is reserved for the special symmetries where a free energy invariant proportional to (Formula presented) is allowed [see L.D. Landau, E.M. Lifshitz, and L.P. Pitaevskii, Electrodynamics of Continuous Media (Pergamon, New York, 1984)]. For the more general couplings, we introduce the term magnetodielectric effects.
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To be completely correct, the expansion in Eq.� 5 should take into account the superexchange nature of (Formula presented) and in the expansion, consider the variations of (Formula presented) with the distances between the magnetic ions and the intermediate diamagnetic ions. However, for the present purposes, Eq.� 5 is sufficient
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To be completely correct, the expansion in Eq.� 5 should take into account the superexchange nature of (Formula presented) and in the expansion, consider the variations of (Formula presented) with the distances between the magnetic ions and the intermediate diamagnetic ions. However, for the present purposes, Eq.� 5 is sufficient.
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