Abstract

AbstractFor certain angles between the magnetic field and the c‐axis of the crystal, “forbidden” magnetic dipolar transitions ΔM = 2, Δm = C, ± 1 (M and m electronic and nuclear azimuthal quantum numbers) can be induced by an axial crystal field in electron paramagnetic resonance. These transitions are observed in ZnS/Mn2+, ZnO/Fe3+, and ZnO/Mn2+ single crystals and compared with theoretical and experimental results.

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