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 />
strained Si layer, with in-plane strain gradient up to 0.5 % along <strong>growth</strong> direction,<br />
and out-<strong>of</strong>-plane GPA strain up to 10 % found to be only near the surface,<br />
which results in a strong tetragonal distortion <strong>of</strong> the coherent InAs <strong>epitaxial</strong><br />
layer. However, this sample showed a weak optical emission at 1153 nm and<br />
it was discussed as defect related transition. The wavelength <strong>of</strong> the observed<br />
peak does not match with direct band gap InAs optical transition. However, the<br />
temperature dependence measurement (Fig. 5.24(b)) conrmed that the observed<br />
peak was not observed at a temperature above 14 K. Fig. 5.24(a) shows the PL<br />
power dependence <strong>of</strong> this transition. All spectra reveal transverse optical (TO)<br />
phonon-assisted exciton emission <strong>of</strong> the Si substrate and barrier at energy <strong>of</strong> 1.1<br />
eV, which is equivalent to a wavelength <strong>of</strong> ∼ 1127 nm.<br />
The indirected emission increased with the excitation power till the saturation.<br />
However, due to the weak connement an additional small thermal energy may let<br />
Figure 5.24: Photoluminescence (PL) measurement <strong>of</strong> 1 ML InAs QDs embedded in<br />
silicon matrix grown on 5 ◦ o-cut (100) substrate. (a) PL power dependence measurement<br />
at 8 K. (b) PL temperature dependence measurement at an excitation power <strong>of</strong><br />
10 W/cm 2 .<br />
the electrons to escape from the connement zone, therefore the optical emission<br />
for this structure was not detected above a temperature <strong>of</strong> 15 K.<br />
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