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Shallow-donor states in spherical quantum dots with parabolic confinement

机译:浅捐助者在球形量子点中具有抛物线限制

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The evidence of a parabolic potential well in quantum wires and dots was reported in the literature, and a parabolic potential is often considered to be a good representation of the "barrier" potential in semiconductor quantum dots. In the present work, the variational and fractional-dimensional space approaches are used in a thorough study of the binding energy of on-center shallow donors in spherical GaAs-Ga{sub}(1-x)Al{sub}xAs quantum dots with potential barriers taken either as rectangular [V{sub}b(eV) = 1.247 x for r > R] or parabolic [V{sub}b(r) = β{sup}2r{sup}2] isotropic barriers. We define the parabolic potential with a β parameter chosen so that it results in the same E{sub}0 ground-state energy as for the spherical quantum dot of radius R and rectangular potential in the absence of the impurity. Calculations using either the variational or fractional-dimensional approaches both for rectangular and parabolic potential result in essentially the same on-center binding energies provided the dot radius is not too small. This indicates that both potentials are alike representations of the quantum-dot barrier potential for a radius R quantum dot provided the parabolic potential is defined with β chosen as mentioned above.
机译:以及在量子线和量子点的抛物线潜在的证据在文献中报道,并且抛物线势经常被认为是在半导体量子点的“屏障”潜在的良好表示。在本工作中,变分和分数尺寸空间方法用于彻底研究球面GAAS-GA}(1-x)Al {Sub} XAS量子点中的中心浅供体的结合能量作为矩形[v {sub} b(EV)= 1.247 x的潜在障碍]或r> r]或抛物线[v {sub} b(r)=β{sup} 2r {sup} 2]各向同性屏障。我们用选择的β参数来定义抛物线电位,使得它在不存在杂质的情况下为半径R和矩形电位的球形量子点导致相同的e {亚} 0接地状态。使用矩形和抛物型电位的变分或分数尺寸方法的计算基本相同的中心绑定能量,条件是点半径不太小。这表明两种电位都是用于半径R量子点的量子点屏障电位的相似表示,所以抛物面电位如上所述用β定义。

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