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The Mechanism of Participation of Non‐Magnetic B‐Site Cations in the Superexchange in Spinels

I. Mayer, Spomenka Ubavkic de ANgelov

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Abstract

Abstract The superexchange between magnetic cations at the A‐sites of spinels with non‐magnetic B‐site cations (e.g. CoAl2O4, Co3O4, CoRh2O4 etc.) is analysed by using a four‐electron, four‐orbital model. The problem is treated in the framework of the CI‐method up to the fourth‐order of the perturbation theory. In the case of Co(III) and Rh(III) in the low‐spin state as B‐site cations four contributions are found: two negative and two positive. One of the ferromagnetic terms is not connected with Hund's rule but has the same origin (delocalization) as the antiferromagnetic ones. The resulting superexchange is always antiferromagnetic. When B is Al3+ there is only one small antiferromagnetic term.

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Abstract The superexchange between magnetic cations at the A‐sites of spinels with non‐magnetic B‐site cations (e.g. CoAl2O4, Co3O4, CoRh2O4 etc.) is analysed by using a four‐electron, four‐orbital model. The problem is treated in the framework of the CI‐method up to the fourth‐order of the perturbation theory. In the case of Co(III) and Rh(III) in the low‐spin state as B‐site cations four contributions are found: two negative and two positive. One of the ferromagnetic terms is not connected with Hund's rule but has the same origin (delocalization) as the antiferromagnetic ones. The resulting superexchange is always antiferromagnetic. When B is Al3+ there is only one small antiferromagnetic term.

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Available abstract

Abstract The superexchange between magnetic cations at the A‐sites of spinels with non‐magnetic B‐site cations (e.g. CoAl2O4, Co3O4, CoRh2O4 etc.) is analysed by using a four‐electron, four‐orbital model. The problem is treated in the framework of the CI‐method up to the fourth‐order of the perturbation theory. In the case of Co(III) and Rh(III) in the low‐spin state as B‐site cations four contributions are found: two negative and two positive. One of the ferromagnetic terms is not connected with Hund's rule but has the same origin (delocalization) as the antiferromagnetic ones. The resulting superexchange is always antiferromagnetic. When B is Al3+ there is only one small antiferromagnetic term.

Key concepts: Superexchange, Antiferromagnetism, Chemistry, Ferromagnetism, Condensed matter physics, Delocalized electron, Magnetic moment, Electron

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