Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
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4.3.3 Optical properties<br />
(a) Photoluminescence<br />
The photoluminescence curves of <strong>Si</strong> 3 N 4 and SRSN (n 1.95eV<br />
= 2.32) samples with<br />
regard to annealing are as shown in gure 4.11. It can be seen that the <strong>Si</strong> 3 N 4<br />
sample exhibits PL of very low intensity between 1.8-2.2 eV, which increases with<br />
annealing. This can be attributed to some radiative <strong>de</strong>fects in the material. The<br />
spectrum was recor<strong>de</strong>d with a 500 nm high pass lter and hence the curve is cut<br />
o after 2.2 eV. No emission is observed from SRSN sample whereas in the Raman<br />
set-up emission was observed from the same sample. The dierence in emission<br />
intensities of these samples when measured in the PL and Raman set-up, can be<br />
attributed to the dierent excitation power <strong>de</strong>nsities used in the experiments (1.4<br />
MW/cm 2 in Raman set-up versus 10 W/cm 2 in the PL set-up).<br />
tel-00916300, version 1 - 10 Dec 2013<br />
(a) <strong>Si</strong> 3 N 4<br />
(b) SRSN<br />
Figure 4.14: Eect of annealing on photoluminescence of <strong>Si</strong> 3 N 4 and SRSN layers.<br />
(λ excitation =488 nm and laser power <strong>de</strong>nsity= 10 W/cm 2 ).<br />
(b) Absorption coecient, (α)<br />
The absorption coecient curves obtained from <strong>Si</strong> 3 N 4 and SRSN as-grown samples<br />
are as presented in gure 4.15.<br />
It can be noticed from this gure that the trend of the absorption coecient<br />
curves are similar to those obtained in samples grown by the rst <strong>de</strong>position approach.<br />
The <strong>Si</strong> 3 N 4 sample has a low absorption in comparison to SRSN samples<br />
and all the curves show a steadily increasing α values with energy as well as with refractive<br />
in<strong>de</strong>x (increasing <strong>Si</strong> excess). The trend of α for this latter case is attributed<br />
to the increase of <strong>Si</strong>-np <strong>de</strong>nsity with <strong>Si</strong> incorporation.<br />
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