2004
DOI: 10.1063/1.1710726
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Energy levels of a parabolically confined quantum dot in the presence of spin-orbit interaction

Abstract: We present a theoretical study of the energy levels in a parabolically confined quantum dot in the presence of the Rashba spin-orbit interaction (SOI). The features of some low-lying states in various strengths of the SOI are examined at finite magnetic fields. The presence of a magnetic field enhances the possibility of the spin polarization and the SOI leads to different energy dependence on magnetic fields applied. Furthermore, in high magnetic fields, the spectra of low-lying states show basic features of … Show more

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Cited by 49 publications
(31 citation statements)
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“…So, controlling and calculating the spin-related effects are attractive and important not only from the fundamental scientific point of view, but also because of their effects on the electronic and optical properties of these structures (Lo 2009;Kuan et al 2004;Winkler 2003;Japaridze et al 2009;Debald and Kramer 2005;Mehdiyev et al 2009;Paaske et al 2010).…”
Section: Introductionmentioning
confidence: 99%
“…So, controlling and calculating the spin-related effects are attractive and important not only from the fundamental scientific point of view, but also because of their effects on the electronic and optical properties of these structures (Lo 2009;Kuan et al 2004;Winkler 2003;Japaridze et al 2009;Debald and Kramer 2005;Mehdiyev et al 2009;Paaske et al 2010).…”
Section: Introductionmentioning
confidence: 99%
“…8,9,10,11,12 However, despite its potential interest for SO coupled low-dimensional systems, the specific 2D Coulomb problem appears to have been only marginally considered in the literature.…”
mentioning
confidence: 99%
“…Equation (2) commutes with the z-projection of the total angular momentum J z =L z + σ z /2, whereL z = −i∂/∂φ, so that the eigenfunctions of (2) can be chosen to be simultaneously eigenfunctions ofĴ z . Since H in polar coordinates allows for separation of variables, its eigenfunctions have therefore the following form: 8,9,10,11,12 Ψ j (r, φ) = f …”
mentioning
confidence: 99%
“…11,37 In several recent works, the Rashba spin-orbit coupling in QD systems was explored by several different groups (see Refs. [38][39][40][41][42]). However, the influence of the coupled magneto-thermoelectroelasticity in QDs has been largely neglected in the literature and we intend to cover this gap.…”
Section: Introductionmentioning
confidence: 99%