Forbidden Transitions (Δ M   2) Induced by an Axial Crystal Field in Electronic Paramagnetic Resonance | Zendy

Marti C. | Zendy; Romestain R. | Zendy; Visocekas R. | Zendy

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Forbidden Transitions (Δ M  2) Induced by an Axial Crystal Field in Electronic Paramagnetic Resonance

Author(s) -

Marti C.,

Romestain R.,

Visocekas R.

Publication year - 1968

Publication title -

physica status solidi (b)

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.51

H-Index - 109

eISSN - 1521-3951

pISSN - 0370-1972

DOI - 10.1002/pssb.19680280109

Subject(s) - hyperfine structure , wurtzite crystal structure , crystal (programming language) , paramagnetism , dipole , condensed matter physics , resonance (particle physics) , field (mathematics) , electron paramagnetic resonance , spin (aerodynamics) , physics , atomic physics , nuclear magnetic resonance , optics , quantum mechanics , mathematics , computer science , diffraction , pure mathematics , thermodynamics , programming language

For certain angles between an applied magnetic field and the optical axis of a crystal, magnetic dipolar transitions Δ M = 2; Δ m = 0, ± 1 ( M and m : electronic and nuclear azimuthal quantum numbers) can be induced by an axial crystal field, including hyperfine interaction. We calculate the corresponding oscillator strengths for a level with effective spin S (2 S + 1 odd). These results can be applied to paramagnetic resonance near g = 4 of Mn ++ in wurtzite.

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