2006 International Conference on Numerical Simulation of Semiconductor Optoelectronic Devices 2006
DOI: 10.1109/nusod.2006.306736
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Effects of Size and Shape on Electronic States of Quantum Dots

Abstract: A strained-modified, single-band, constant-potential three-dimensional model is formulated to study the dependence of electronic states of InAs/ GaAs quantum dots ͑QDs͒ on shape and size variation. The QD shapes considered are ͑i͒ cuboid, ͑ii͒ cylindrical, ͑iii͒ pyramidal, ͑iv͒ conical, and ͑v͒ lens shaped. Size variations include ͑i͒ QD volume ͑ii͒ QD base length, and ͑iii͒ QD height, taking into account aspect ratio variation. Isovolume QD shapes with narrow tips were found to have higher ground-state energi… Show more

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Cited by 10 publications
(17 citation statements)
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“…where cylindrical coordinates (ρ, θ) are the distance and angle describing the position of an electron in the plane perpendicular to the electric field; F is external electric field applied in the z-direction; m* is the effective mass of the electron, V(ρ,z)=1/2m*ω 2 Because of the axial symmetry of the system, angular momentum projection onto the z axis is conserved L z =ℏ m (m=0, 1, 2, …-magnetic quantum number), and their eigenfunctions exp(imz) determine the dependence of the unknown electron wave function versus an angle:…”
Section: Theoretical Backgroundmentioning
confidence: 99%
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“…where cylindrical coordinates (ρ, θ) are the distance and angle describing the position of an electron in the plane perpendicular to the electric field; F is external electric field applied in the z-direction; m* is the effective mass of the electron, V(ρ,z)=1/2m*ω 2 Because of the axial symmetry of the system, angular momentum projection onto the z axis is conserved L z =ℏ m (m=0, 1, 2, …-magnetic quantum number), and their eigenfunctions exp(imz) determine the dependence of the unknown electron wave function versus an angle:…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…Since Bastard calculated [1] for the very first time the impurity binding energy in QW many works on this subject have been published. Over the last three decades, new calculation methods have been developed to determine the binding energy of IS in QWs and QDs, by assuming the form of confinement potential [2][3][4][5] and the features of the band structure [5][6][7][8][9]. The form of the confinement potential is a significant characteristic.…”
Section: Introductionmentioning
confidence: 99%
“…We also employ the finite barrier model as the infinite barrier EMA model with 1/R 2 scaling of the kinetic term has been shown to be inaccurate by over-estimating the band gaps for sizes where the confinement are significant [Sapra et al, 2003, Kayanuma andMomiji, 1990]. The finite barrier has been shown to be accurate and widely adopted with the single-particle finite well effective mass approximation model [Pellegrini et al, 2005, Zhang and Sharma, 2005, Ngo et al, 2006. Thus the finite depth/width square well EMA (FWEMA) method [Pellegrini et al, 2005, Baskoutas and Terzis, 2008, Marin et al, 1998] and the numerical finite element approach are used here to solve the Schrödinger equation,…”
Section: Effective Volume Modelmentioning
confidence: 99%
“…Using numerical simulations, Fonoberov and Pokatilov [2002] Li et al [2001a] fitted the transition energies with volume, ∆E g ≈ V −γ o , to obtain the value of γ of 0.38 for disk shape, 0.35 for ellipsoidal lens shape, 0.31 for cut spherical lens shape, and 0.27 for cone shape. Ngo et al [2006] introduced the effective volume by replacing…”
Section: Introductionmentioning
confidence: 99%
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