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Exciton magnetic polaron in semimagnetic semiconductor nanocrystals
109
Citations
25
References
1997
Year
Categoryquantum ElectronicsEngineeringMagnetic ResonanceSpintronic MaterialSemiconductor NanostructuresSemiconductorsMagnetismPolariton DynamicQuantum MaterialsEquilibrium Polaron SizeQuantum SciencePhysicsQuantum DeviceExciton Magnetic PolaronNanocrystalline MaterialQuantum MagnetismSpintronicsNatural SciencesApplied PhysicsCondensed Matter PhysicsMagnetic PolaronQuantum Dot Radius
We present a theoretical study of the magnetic polaron associated with an electron-hole pair in a diluted magnetic semiconductor quantum dot. It is based on the effective-mass approximation in the strong confinement regime, which incorporates the coupling between the light- and heavy-hole bands. The magnetic polaron, arising from the sp-d exchange interaction between the confined carriers and the magnetic ions, is treated in a self-consistent mean-field approach that leads to coupled nonlinear Schr\"odinger equations for the electron and the hole. The local response to the effective field is modeled by the experimental high-field magnetization curve in the bulk. The electron-hole Coulomb interaction is taken into account. An exact numerical solution of the three coupled equations is used to calculate the equilibrium polaron size, binding energy (${\mathrm{E}}_{\mathrm{p}}$), and spin (${\mathrm{S}}_{\mathrm{p}}$). Results are first presented for ${\mathrm{Cd}}_{1\mathrm{\ensuremath{-}}\mathrm{x}}$${\mathrm{Mn}}_{\mathrm{x}}$Te nanocrystals with x=0.11. ${\mathrm{E}}_{\mathrm{p}}$ decreases and the orbital contraction increases with an increasing quantum dot radius (a). In small dots, approaching saturation in the core region, ${\mathrm{E}}_{\mathrm{p}}$ decreases slowly as the temperature (T) increases. In large dots ${\mathrm{E}}_{\mathrm{p}}$(T) decreases rapidly towards the fluctuation regime, where ${\mathrm{E}}_{\mathrm{p}}$\ensuremath{\propto}${\mathrm{a}}^{\mathrm{\ensuremath{-}}3}$. A similar temperature dependence is obtained for ${\mathrm{S}}_{\mathrm{p}}$; the fluctuation-regime value is, however, size independent. The light-induced magnetization enhancement due to polaron formation is considered and an optimal quantum dot radius is predicted to be \ensuremath{\sim}30 \AA{}. We have also calculated ${\mathrm{E}}_{\mathrm{p}}$ as a function of an applied magnetic field, which shows a decreasing behavior that depends on a and T. Theoretical results for ${\mathrm{Cd}}_{1\mathrm{\ensuremath{-}}\mathrm{x}}$${\mathrm{Mn}}_{\mathrm{x}}$Se nanocrystals show a good agreement with recently reported experimental data on the photoluminescence Stokes shift versus magnetic field.
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