The alkali hyperoxides AO₂ exhibit elastic and magnetic interactions due to the nature of the diatomic molecule ion O₂^-. These anion sublattices represent simple magnetic spin-{} systems. In contrast to $3d$- or $4f$-electron systems, where magnetoelastic interactions induce magnetostriction, the (2p)π-electron system KO₂ exhibits magnetogyration. A crystallographic phase transition involving a considerable change in the molecular orientation can be induced by an applied magnetic field. A theoretical model based on the exchange modulation produced by this reorientation describes the salient features.
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Bösch et al. (1980) studied this question.
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