Evolution of InAs/GaAs(001) islands during the two- to three-dimensional growth mode transition in molecular-beam epitaxy

2007 ◽  
Vol 18 (16) ◽  
pp. 165301 ◽  
Author(s):  
J Wu ◽  
P Jin ◽  
Y H Jiao ◽  
X J Lv ◽  
Z G Wang
2000 ◽  
Vol 9 (3-6) ◽  
pp. 506-511 ◽  
Author(s):  
B. Daudin ◽  
G. Feuillet ◽  
Guido Mula ◽  
H. Mariette ◽  
J.L. Rouvière ◽  
...  

2019 ◽  
Vol 19 (4) ◽  
pp. 542-547
Author(s):  
Agata Jasik ◽  
Iwona Sankowska ◽  
Andrzej Wawro ◽  
Jacek Ratajczak ◽  
Dariusz Smoczyński ◽  
...  

1995 ◽  
Vol 395 ◽  
Author(s):  
U. Rossner ◽  
J.-L. Rouviere ◽  
A. Bourret ◽  
A. Barski

ABSTRACTElectron Cyclotron Resonance Plasma Assisted Molecular Beam Epitaxy (ECR-MBE) and Gas Source Molecular Beam Epitaxy (GSMBE) have been used to grow hexagonal GaN on Si (111). In the ECR-MBE configuration high purity nitrogen has been used as nitrogen source. In GSMBE ammonia was supplied directly to the substrate to be thermally cracked in the presence of gallium.By a combined application of in-situ reflection high-energy electron-diffraction (RHEED) and cross-sectional transmission electron microscopy (TEM) the growth mode and structure of GaN were determined. The growth mode strongly depends on growth conditions. Quasi two dimensional growth was observed in ECR-MBE configuration for a substrate temperature of 640°C while three dimensional growth occured in GSMBE configuration in the temperature range from 640 to 800°C.Low temperature (9 K) photoluminescence spectra show that for samples grown by ECR-MBE and GSMBE a strong near band gap emission peak dominates while transitions due to deep level states are hardly detectable. The best optical results (the highest near band gap emission peak intensity) have been observed for samples grown by GSMBE at high temperature (800°C). This could be explained by the increase of grain dimensions (up to 0,3 – 0,5 μm) observed in samples grown by GSMBE at 800°C.


1994 ◽  
Author(s):  
Masahiro Yoshikawa ◽  
Takashi Nomura ◽  
Kenji Ishikawa ◽  
Minoru Hagino

1993 ◽  
Vol 318 ◽  
Author(s):  
Xiaochuan Zhou ◽  
Wiley P. Kirk

ABSTRACTThe crystalline quality of ZnS films grown on arsenic covered Si(100) surfaces is shown to be improved as compared to films grown on bare silicon surfaces by MBE (molecular beam epitaxy). Employing RGA (residual gas analyzer) and RHEED (reflection high energy electron diffraction) techniques, we found that a strong initial adsorption of sulfur on bare silicon surfaces led to the formation of disordered silicon-sulfide surfaces. This disordered surface initiated three-dimensional growth of ZnS and resulted in poor crystalline quality. An arsenic overlayer was found to be effective in preventing the interaction of sulfur with the silicon surface and thereby maintained surface ordering. X-ray rocking curve analysis indicated higher crystallinity in ZnS films grown on arsenic covered surfaces.


1994 ◽  
Vol 351 ◽  
Author(s):  
H. Gossner ◽  
G. Fehlauer ◽  
W. Kiunke ◽  
I. Eisele ◽  
M. Stolz ◽  
...  

ABSTRACTAs reported previously, perfect facets can be achieved at the side walls of submicron silicon mesa structures grown by molecular beam epitaxy (MBE) with micro shadow masks [1]. An essentially self organizing, three-dimensional growth was observed. In this paper we present the results of the epitaxial growth on (001) substrates using long (≥ 1μm), lineshaped mask apertures, which put constraints on the formation of facets. At a growth temperature of 500°C {111} facet formation is observed for lineshaped mesas oriented along the <110> direction of the substrate. Side walls with a length of I μm are perfectly plane, while mesas with a length of 10 μm and more show rough sidewalls. This is explained by a limited silicon adatom diffusion on the facet. For higher flux rates the facet formation is suppressed. This can be understood in terms of a reduced adatom diffusion.A crossover from {111} to {113} facet formation is observed at growth temperatures above 500°C. A model for the temperature dependent formation of {111} and {113} facets is given.


1993 ◽  
Vol 63 (6) ◽  
pp. 821-823 ◽  
Author(s):  
H. Toyoshima ◽  
T. Niwa ◽  
J. Yamazaki ◽  
A. Okamoto

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