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- W2322693931 abstract "Electronic Raman transitions due to the spin flip of the $3d$ electrons of ${mathrm{Co}}^{2+}$ in ${mathrm{Zn}}_{1ensuremath{-}x}{mathrm{Co}}_{x}mathrm{Te}$ and ${mathrm{Cd}}_{1ensuremath{-}x}{mathrm{Co}}_{x}mathrm{Te} (x<~0.01)$ are observed at $ensuremath{Elzxh}{ensuremath{omega}}_{mathrm{PM}}=g({mathrm{Co}}^{2+}){ensuremath{mu}}_{B}H$ with $g({mathrm{Co}}^{2+})=2.295ifmmodepmelsetextpmfi{}0.010$ and $2.310ifmmodepmelsetextpmfi{}0.002,$ respectively. The intensity of Raman electron paramagnetic resonance (Raman-EPR) shows strong resonant enhancement when the incident or scattered photon energy coincides with that of a Zeeman component of the free exciton. Under resonant conditions, the Raman spectra display ``ZnTe-like'' (or ``CdTe-like'') and ``CoTe-like'' longitudinal optical (LO) phonons in combination with the spin-flip transitions, a consequence of the Frohlich interaction. In ${mathrm{Zn}}_{1ensuremath{-}x}{mathrm{Co}}_{x}mathrm{Te},$ even the ZnTe-like TO phonon exhibited EPR sidebands but mediated by the deformation potential; the large $pensuremath{-}d$ spin-spin exchange interaction in ${mathrm{Co}}^{2+}$-based II-VI diluted magnetic semiconductors is the underlying microscopic mechanism." @default.
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- W2322693931 date "2001-03-13" @default.
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- W2322693931 title "Raman electron paramagnetic resonance in<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>Zn</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mi>−</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=normal>Co</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi mathvariant=normal>Te</mml:mi></mml:math>and<mml:math …" @default.
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- W2322693931 doi "https://doi.org/10.1103/physrevb.63.125208" @default.
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