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Dependence of the electronic structure of self-assembled InGaAs/GaAs quantum dots on height and composition

机译:自组装InGaas / Gaas的电子结构的依赖性   量子点的高度和成分

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摘要

While electronic and spectroscopic properties of self-assembledIn_{1-x}Ga_{x}As/GaAs dots depend on their shape, height and alloycompositions, these characteristics are often not known accurately fromexperiment. This creates a difficulty in comparing measured electronic andspectroscopic properties with calculated ones. Since simplified theoreticalmodels (effective mass, k.p, parabolic models) do not fully convey the effectsof shape, size and composition on the electronic and spectroscopic properties,we offer to bridge the gap by providing accurately calculated results as afunction of the dot height and composition. Prominent results are thefollowing. (i) Regardless of height and composition, the electron levels formshells of nearly degenerate states. In contrast, the hole levels form shellsonly in flat dots and near the highest hole level (HOMO). (ii) In alloy dots,the electrons' ``s-p'' splitting depends weakly on height, while the ``p-p''splitting depends non-monotonically. In non-alloyed InAs/GaAs dots, both thesesplittings depend weakly on height. For holes in alloy dots, the ``s-p''splitting decreases with increasing height, whereas the ``p-p'' splittingremains nearly unchaged. Shallow, non-alloyed dots have a ``s-p'' splitting ofnearly the same magnitude, whereas the ``p-p'' splitting is larger. (iii) Asheight increases, the ``s'' and ``p'' character of the wavefunction of the HOMObecomes mixed, and so does the heavy- and light-hole character. (iv) In alloydots, low-lying hole states are localized inside the dot. Remarkably, innon-alloyed InAs/GaAs dots these states become localized at the interface asheight increases. This localization is driven by the biaxial strain present inthe nanostructure.
机译:尽管自组装In_ {1-x} Ga_ {x} As / GaAs点的电子和光谱性质取决于它们的形状,高度和合金成分,但是从实验中常常无法准确地了解这些特征。这就很难将测得的电子和光谱性质与计算得出的性质进行比较。由于简化的理论模型(有效质量,k.p,抛物线模型)不能完全传达形状,尺寸和成分对电子和光谱性质的影响,因此我们提供了通过根据点高和成分而精确计算的结果来弥合间隙。出色的结果如下。 (i)不论高度和组成如何,电子能级形成几乎简并状态的壳。相反,孔位仅在平面点中且在最高孔位(HOMO)附近形成壳。 (ii)在合金点中,电子的``s-p''分裂弱依赖于高度,而``p-p''分裂非单调依赖。在非合金InAs / GaAs点中,这两种分解都很少依赖于高度。对于合金点中的孔,随着高度的增加,``s-p''裂变减少,而``p-p''裂变几乎保持未破裂状态。浅的非合金圆点的``s-p''分裂几乎相同,而``p-p''分裂则更大。 (iii)Asheight增加,HOMO的波函数的``s''和``p''特征混合,重孔和轻孔特征也是如此。 (iv)在合金点中,低洼的孔态位于点内部。值得注意的是,非合金InAs / GaAs点的这些状态局限在界面上,重心增加。这种定位是由纳米结构中存在的双轴应变驱动的。

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