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Neutral manganese acceptor in GaP: An electron-paramagnetic-resonance study
68
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1996
Year
EngineeringMagnetic ResonanceAbsorption SpectroscopyElectronic Excited StateMagnetoresistanceMagnetismElectron SpectroscopyOptical PropertiesElectron Paramagnetic ResonanceQuantum MaterialsPhysicsQuantum ChemistryNeutral Manganese AcceptorMn AcceptorQuantum MagnetismSpintronicsFerromagnetismNatural SciencesSpectroscopyCondensed Matter PhysicsApplied PhysicsThermal EquilibriumNeutral Mn AcceptorLight Absorption
In order to clarify the nature of the neutral Mn acceptor in GaP, we have carried out optical-absorption and electron-paramagnetic-resonance (EPR) experiments using both conventional and thermally detected EPR on semi-insulating GaP:Mn. In thermal equilibrium at low temperatures, all the manganese occurs in the charged acceptor state ${\mathrm{Mn}}_{\mathrm{Ga}}^{2+}$(${\mathit{A}}^{\mathrm{\ensuremath{-}}}$). By illumination with photon energies greater than 1.2 eV, it can be partially converted into the neutral charge state. The arising photostimulated EPR spectrum shows the characteristic of a tetragonally distorted center with an integer spin. The resonance lines are detectable only at temperatures below 7 K, and their linewidth of about 50 mT is due to the unresolved Mn-hyperfine splitting. We interpret the experimental data in terms of ${\mathrm{Mn}}_{\mathrm{Ga}}^{3+}$ ions on strain-stabilized sites of tetragonal symmetry due to a strong T\ensuremath{\bigotimes}\ensuremath{\epsilon} Jahn-Teller coupling within the $^{5}$${\mathit{T}}_{2}$ ground state. Such a behavior is expected for a 3${\mathit{d}}^{4}$ defect, as observed for the isoelectronic impurity ${\mathrm{Cr}}^{2+}$ in GaAs, and other tetrahedrally coordinated semiconductors. The analysis of the EPR spectra thus verifies that, in GaP, the neutral charge state of the Mn acceptor is ${\mathrm{Mn}}_{\mathrm{Ga}}^{3+}$(${\mathit{A}}^{0}$) in contrast to its behavior in GaAs and InP. \textcopyright{} 1996 The American Physical Society.
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