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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MBE Growth <strong>of</strong> Self-Assembled InAs and InGaAs Quantum Dots Embedded in<br />
Silicon Matrix<br />
Figure 5.8:<br />
(1 × 1 µm 2 ) AFM images <strong>of</strong> 2 MLs <strong>of</strong> InAs QDs grown using SK mode<br />
with dierent indium (In) <strong>growth</strong> rates (a) 108 nm/h (circular InAs QDs) and (b) 324<br />
nm/h (dash-like QDs).<br />
The observed shape transition is due to the preferential migration <strong>of</strong> indium<br />
atoms along [110] crystal direction, resulted from the anisotropic migration<br />
lengths <strong>of</strong> indium atoms [85].<br />
Fig. 5.9 shows the dependence <strong>of</strong> dierent <strong>growth</strong> parameters on their main<br />
structural properties such as density, lateral size, height <strong>of</strong> InAs QDs.<br />
From<br />
this study, one can conclude that the optimized <strong>growth</strong> parameters <strong>of</strong> InAs QDs<br />
can be identied morphology wise. The <strong>growth</strong> temperature should be set below<br />
450 ◦ C, which is an essential condition for InAs QDs formation and can avoid any<br />
additional indium desorption, which is signicantly starts above this temperature<br />
[3]. A low <strong>growth</strong> rate <strong>of</strong> 108 nm/h resulted in circular QDs shape formation.<br />
However, average dots densities with non-overlapping dots can be achieved with<br />
a V/<strong>III</strong> ratio <strong>of</strong> 25 as well as with an InAs coverage less than 5 MLs.<br />
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