Analysis of Faceted Growth Hillocks in MOCVD Grown Epitaxial HgCdTe on GaAs with a Nuclear Microprobe

1991 ◽  
Vol 238 ◽  
Author(s):  
David N. Jamieson ◽  
S. P. Dooley ◽  
S. P. Russo ◽  
P. N. Johnston ◽  
G. N. Pain ◽  
...  

ABSTRACTHg1-xCdxTe epitaxial layers on GaAs substrates grown by Metal Organic Chemical Vapour Deposition (MOCVD) display growth defects resembling pyramidal faceted hillocks which appear to originate from defects originally present on the substrate. For <100> oriented GaAs substrates and normal growth conditions, these growth defects have an areal density of 1–1000 mm-2. The size of the hillocks depends on the layer thickness and they have the potential to degrade performance of optoelectronic devices fabricated in the epitaxial layers. Nuclear microprobe analysis, performed with a 2 MeV He+ beam focused to less than 5 μm in diameter, has allowed the hillocks to be imaged with the technique of Channeling Contrast Microscopy (CCM). Channeling spectra, obtained by Rutherford Backseat tering Spectrometry (RBS) of the hillocks themselves, showed that the χmin was 13 %. This was similar to the χmin of the high quality single crystal surrounding material. The CCM images also revealed extensive regions of poor channeling, with shapes that suggested that the regions originally arose from scratches in the substrate. These poor channeling regions were not readily observable by other techniques.

2019 ◽  
Vol 52 (3) ◽  
pp. 637-642 ◽  
Author(s):  
Jiang-Dong Gao ◽  
Jian-Li Zhang ◽  
Xin Zhu ◽  
Xiao-Ming Wu ◽  
Chun-Lan Mo ◽  
...  

The growth mechanism of V-defects in GaN films was investigated. It was observed that the crystal faces of both the sidewall of a V-defect and the sidewall of the GaN film boundary belong to the same plane family of \{ {{{10\bar 11}}} \}, which suggests that the formation of the V-defect is a direct consequence of spontaneous growth like that of the boundary facet. However, the growth rate of the V-defect sidewall is much faster than that of the boundary facet when the V-defect is filling up, implying that lateral growth of \{ {{{10\bar 11}}} \} planes is not the direct cause of the change in size of V-defects. Since V-defects originate from dislocations, an idea was proposed to correlate the growth of V-defects with the presence of dislocations. Specifically, the change in size of the V-defect is determined by the growth rate around dislocations and the growth rate around dislocations is determined by the growth conditions.


1991 ◽  
Vol 69 (3-4) ◽  
pp. 412-421 ◽  
Author(s):  
P. Cova ◽  
R. A. Masut ◽  
J. F. Currie ◽  
A. Bensaada ◽  
R. Leonelli ◽  
...  

The development of a low pressure, horizontal MOCVD (metal-organic chemical vapour deposition) reactor has allowed us to study the effect of phosphine and trimethylindium molar fluxes on the epitaxial growth of InP. Study of the growth rate in the temperature range 550–620 °C shows that the growth can be limited by the reaction kinetics at the surface. Epitaxial layers of good morphological quality have been obtained by reducing the rate of growth even if the growth is limited by the reaction kinetics at the surface. The variation of the electronic mobility with the PH3 molar flux reveals the existence of an optimum mobility region, even with a constant V: III ratio. Photoluminescence experiments carried out on the samples show the good crystallographic quality of the epitaxial layers. Spectra taken in the energy range 0.8–1.2 eV show the evolution of two structures at 0.91 and 1.08 eV that we associate with an antisite PIn and a VIn defect, respectively.[Journal translation]


2006 ◽  
Vol 6 (11) ◽  
pp. 3325-3328 ◽  
Author(s):  
Jeong-Hun Kim ◽  
Yong-Chul Jung ◽  
Sang-Hee Suh ◽  
Jin-Sang Kim

Metal organic chemical vapour deposition (MOCVD) has been investigated for growth of Bi2Te3 and Sb2Te3 films on (001) GaAs substrates using trimethylbismuth, triethylantimony and diisopropyltelluride as metal organic sources. The surface morphologies of Bi2Te3 and Sb2Te3 films were strongly dependent on the deposition temperatures as it varies from a step-flow growth mode to island coalescence structures depending on deposition temperature. In-plane carrier concentration and electrical Hall mobility were highly dependent on precursor ratio of VI/V and deposition temperature. By optimizing growth parameters, we could clearly observe an electrically intrinsic region of the carrier concentration over the 240 K in Bi2Te3 films. The high Seebeck coefficient (of −160 μVK−1 for Bi2Te3 and + 110 μVK−1 for Sb2Te3 films, respectively) and good surface morphologies of these materials are promising for the fabrication of a few nm thick periodic Bi2Te3/Sb2Te3 super lattice structures for thin film thermoelectric device applications.


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