28.02.2014 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

5.4 Self-Assembled InAs QDs Embedded in Si Matrix<br />

negligible strain relaxation (Eq. 5.10) and negligible crystal rotation. However,<br />

by direct substitution <strong>of</strong> the approximation in Eq. 5.10 into Eq. 5.11, the relation<br />

between material strain and GPA strain is obtained and expressed by Eq. 5.12:<br />

d bulk<br />

Si<br />

d measured<br />

Si<br />

= 1 (approximation) (5.10)<br />

ε GP A − f<br />

1 + f<br />

=<br />

d measured<br />

InAs (<br />

d bulk<br />

Si<br />

d measured<br />

Si<br />

d bulk<br />

InAs<br />

) − d bulk<br />

Si<br />

(5.11)<br />

ε InAs = εGP A − f<br />

1 + f<br />

(5.12)<br />

The material strain analysis <strong>of</strong> dierent shape and size InAs QDs is shown in<br />

Fig. 5.27. The direction and magnitude <strong>of</strong> tensile and compressive strain is clearly<br />

shown with the color map. The color scale indicates the type and magnitude <strong>of</strong><br />

the strain.<br />

The tensile strain has positive sign values (marked in red to yellow colors<br />

in Fig. 5.27) and is pointing to outward directions (highlighted by red arrows).<br />

Fig. 5.27(a) shows an example <strong>of</strong> tensile strain in y direction (ε yy ). On the other<br />

hand, the compressive strain has negative sign values and marked in green to<br />

dark blue colors with direction (highlighted by red arrows) pointing to inward<br />

direction as illustrated in Fig. 5.27(b). The structure <strong>of</strong> 4 MLs InAs embedded in<br />

Si matrix proved to have high degree <strong>of</strong> relaxation and low residual strain values.<br />

The bulk lattice mismatch <strong>of</strong> 11.55 % is relieved by dislocation loops along the<br />

interface consisting <strong>of</strong> perfect 60 ◦ -type dislocations and partial dislocation with<br />

stacking faults inside the InAs clusters, which is in agreement with the literature<br />

[1]. By two-dimensional strain mapping derived from high-resolution TEM<br />

structure images, no strain gradients in the Si matrix around InAs clusters are<br />

detectable (Fig. 5.26). Therefore, it has been observed that the strain relaxation<br />

eects is mostly relieved by defects formation inside InAs QDs such as (SFs and<br />

MTs) and mist dislocation (MD) array at the InAs/Si interface, as it was shown<br />

in Fig. 5.27. On the other hand, anisotropic distortion <strong>of</strong> InAs lattice constant<br />

is another indication <strong>of</strong> strain relaxation. The residual strain is discussed based<br />

on the thermal mismatch between InAs and Si. However, the deformation force<br />

93

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!