Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
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patterns indicating a 2D smooth surface construction prior to the<br />
MBE <strong>growth</strong>.<br />
The evolution <strong>of</strong> size, density and shape <strong>of</strong> the QDs are ex-situ characterized<br />
by atomic-force microscopy (AFM) and transmission electron<br />
microscopy (TEM). The InAs QDs density is strongly increased<br />
from 10 8 to 10 11 cm −2 at V/<strong>III</strong> ratios in the range <strong>of</strong> 15-35 (<strong>beam</strong><br />
equivalent pressure values). InAs QD formations are not observed<br />
at temperatures <strong>of</strong> 500 ◦ C and above. Growth experiments on (111)<br />
substrates show orientation dependent QD formation behaviour. A<br />
signicant shape and size transition with elongated InAs quantum<br />
dots and dashes has been observed on (111) orientation and at higher<br />
Indium-<strong>growth</strong> rate <strong>of</strong> 0.3 ML/s. The 2D strain mapping derived<br />
from high-resolution TEM <strong>of</strong> InAs QDs embedded in silicon matrix<br />
conrmed semi-coherent and fully relaxed QDs embedded in defectfree<br />
silicon matrix. The strain relaxation is released by dislocation<br />
loops exclusively localized along the InAs/Si interfaces and partial<br />
dislocations with stacking faults inside the InAs clusters.<br />
The site controlled <strong>growth</strong> <strong>of</strong> GaAs/In 0.15 Ga 0.85 As/GaAs nanostructures<br />
has been demonstrated for the rst time with 1 µm spacing and<br />
very low nominal deposition thicknesses, directly on pre-patterned Si<br />
without the use <strong>of</strong> SiO 2 mask.<br />
Thin planar GaP layer was successfully grown through migration enhanced<br />
epitaxy (MEE) to initiate a planar GaP wetting layer at the<br />
polar/non-polar interface, which work as a virtual GaP substrate, for<br />
the GaP-MBE subsequently <strong>growth</strong> on the GaP-MEE layer with total<br />
thickness <strong>of</strong> 50 nm. The best root mean square (RMS) roughness<br />
value was as good as 1.3 nm. However, these results are highly encouraging<br />
for the realization <strong>of</strong> <strong>III</strong>-V optical devices on silicon for<br />
potential applications.