J. C. Ferrer, F. Peiró, A. Cornet, J. Morante, T. Utzmeier, F. Briones
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引用次数: 1
摘要
本文报道了在相对低温(330°C < T < 400°C)下,通过原子层分子束外延在InP衬底上生长的Insb外延薄膜的结构表征。此外,我们还研究了引入分子束外延生长的中间Insb/InP缓冲层的影响。利用透射电子显微镜(TEM)和热透射电子显微镜(HRTEM)研究了缺陷的密度和性质,以及两种晶格失配较大(10.4%)的层之间的调节机制。结果表明,无论采用何种生长方式,无论有无缓冲层,在界面附近缺陷密度都较高,但随着生长的进行,得到的层质量较好。这两种样品的主要缺陷类型是穿线位错和层错,但中间层的引入导致两种复杂的三维缺陷的形成,包括晶体取向错误,这导致Insb层的异常生长,导致不同的生长速率和表面形成锥体或截锥体丘。在这种情况下,还使用扫描电子显微镜和拉曼分析来研究缺陷对表面形貌的影响并确定其结构。此外,在该样品中还注意到层错分布的各向异性:(l10)-(ill)A滑动面的密度高于(l10)-(ill)B滑动面的密度。由于大的晶格错配而引起的应变在两种样品中都被
Microstructure of Pyramidal Defects in InSb Layers Grown by Atomic Layer Molecular Beam Epitaxy on InP Substrates
We report on the structural characterization of epitaxial Insb films grown on InP substrates by atomic layer molecular beam epitaxy at relatively low temperatures (330 °C < T < 400 °C). Moreover, we study the effect of the introduction of an interme- diate Insb/InP buffer layer grown by molecular beam epitaxy. The studies were carried out by TEM and HRTEM, to investigate the densities and nature of the defects and the accommoda- tion mechanism between the two types of layers which have a large lattice mismatch (10.4%). Results show a high defect density at the interface vicinity whatever the growth method em- ployed, with or without buffer layers, but better quality layers are obtained as growth proceeds. The prevailing type of defects are threading dislocations and stacking faults for both types of samples, but the introduction of the intermediate layers leads to the formation of two types of complex three-dimensional defects, consisting m crystal misorientations, that induce an anoma- lous growth of the Insb layer leading to different growth rates and the formation of pyramidal or truncated pyramidal hillocks on the surface. In this case scanning electron microscopy and Raman analysis were also performed to study the influence of the defects on surface morphology and confirm their structure. Moreover, anisotropy of the stacking fault distribution is noticed in this sample: the density for (l10)-(ill)A slip planes is higher than for the (l10)-(ill)B slip planes. Strain due to large lattice mismatch is relieved m both types of samples by the