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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5.4 Self-Assembled InAs QDs Embedded in Si Matrix<br />
Figure 5.13: TEM cross-section image <strong>of</strong> 2 MLs InAs QDs embedded in silicon matrix<br />
grown on 5 ◦ o-cut (100) substrate. (a) Dark eld cross section TEM image with narrow<br />
dots size distribution. (b) HR-TEM cross-section image with dierent dots shapes.<br />
(TEM performed@PDI-Berlin).<br />
The Moiré fringes pattern inside the dots in Fig. 5.13(b) reveal a good crystal<br />
quality <strong>of</strong> some dots, especially dots with more than one facet, hence spherical<br />
dots, seem to have more defects. Another interesting feature <strong>of</strong> the InAs islands on<br />
Si observed in Fig. 5.12(c) is the shift <strong>of</strong> the interface toward the InAs islands, and<br />
this interface is dened as the location where the extra half plane <strong>of</strong> dislocation is<br />
terminated. The interface shift has also been observed in the lower magnication<br />
TEM [17]. One possible explanation <strong>of</strong> a shift <strong>of</strong> 3 MLs Si to the InAs island<br />
in Fig. 5.12(c) is the interaction between dislocations and the inevitable ones<br />
parallel to the image plane [1]. The dislocations parallel to the image plane repel<br />
the ones to reach the interface. In this case the dislocations may be pinned above<br />
the interface and cause such a shift. The dislocations shown in Fig. 5.12(c) are<br />
not located precisely at the interface. If this is true, the precise location <strong>of</strong> the<br />
interface, which is a challenging subject in such nanometer scale structures, will<br />
have to be dened by a criterion rather than the location <strong>of</strong> dislocations [1].<br />
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