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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(d) Photoluminescence<br />
Figure 3.14a shows the PL spectra of SRSO-P15 at various annealing treatments.It<br />
can be seen that there is no emission whatever be the annealing conditions. The<br />
absence of PL may be attributed to high <strong>Si</strong> excess due to any/all of the following<br />
processes:<br />
(i) an increase in the non-radiative paths in the matrix.<br />
(ii) a higher disor<strong>de</strong>r in the matrix as observed by FTIR investigations.<br />
(iii) possible formation of oversized <strong>Si</strong>-np upon annealing, leading to the loss of<br />
quantum connement eect.<br />
tel-00916300, version 1 - 10 Dec 2013<br />
(a) PL spectra vs. annealing of SRSO-P15.(b) PL intensity vs. n 1.95eV<br />
of Method 3 SRSO.<br />
Figure 3.14: PL spectra of (a) SRSO-P15 sample at various annealing and (b) Other<br />
SRSO samples grown by method 3 but with lower refractive in<strong>de</strong>x.(*) indicates second<br />
or<strong>de</strong>r laser emission.<br />
This is conrmed by the presence of luminescence witnessed in other samples<br />
grown using method 3, that have lower refractive in<strong>de</strong>x and therefore lower <strong>Si</strong> excess<br />
in the matrix (Fig. 3.14b).<br />
(e) Absorption coecient<br />
The values of absorption coecients (α) between 1.5-4.5 eV were extracted from k<br />
values obtained by ellipsometry measurements as <strong>de</strong>tailed in section 2.2.6 of chapter<br />
2. Figure 3.15 represents the absorption coecient curves of SRSO-P15 before and<br />
after dierent annealing treatments.<br />
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