Non-linear optical response of an impurity in a cylindrical quantum dot under the action of a magnetic field

The linear and nonlinear optical response in a cylindrical quantum dot (CQD) of GaAs/Ga0.6Al0.4As with a donor impurity in a uniform magnetic field applied in the axial direction of the cylinder is studied theoretically. The calculations were carried out in approximations of effective mass and two-l...

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Bibliographic Details
Published inPhysica. B, Condensed matter Vol. 511; pp. 68 - 73
Main Authors Portacio, Alfonso A., Rodríguez, Boris A., Villamil, Pablo
Format Journal Article
LanguageEnglish
Published Amsterdam Elsevier B.V 15.04.2017
Elsevier BV
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Summary:The linear and nonlinear optical response in a cylindrical quantum dot (CQD) of GaAs/Ga0.6Al0.4As with a donor impurity in a uniform magnetic field applied in the axial direction of the cylinder is studied theoretically. The calculations were carried out in approximations of effective mass and two-level quantum systems. Using the variational method, the binding energies and the wave functions of the 1s-like y 2pz-like states for different positions of the impurity inside the CQD were found. It was found that the binding energy is greatest in the center of the CQD and diminishes as the impurity moves radially and/or axially. The optical rectification, the change in the refractive index, and the optical absorption were studied as functions of the energy of a photon incident on the CQD and different intensities of the magnetic field, with an impurity located at various positions. It was found that in a CDQ with an impurity inside, the effect of the variation of the intensity of the magnetic field on the optical response is much less than the effect produced by the variation of the position of the impurity. The physical reason for this behavior is that in nanostructures with impurities the Coulomb confinement is stronger than the magnetic confinement. It was also found that when the impurity is in the center of the quantum dot, the optical rectification coefficient is zero, due to the symmetry that the wave function of the impurity exhibits at this geometric point. When the impurity moves in the axial direction, the symmetry is broken and the optical rectification coefficient is different from zero, and its value increases as the impurity moves away from the center of the CQD.
ISSN:0921-4526
1873-2135
DOI:10.1016/j.physb.2017.02.008