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 ...
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
(a) Fourier transform infrared spectroscopy<br />
tel-00916300, version 1 - 10 Dec 2013<br />
Figure 3.11 shows the FTIR spectra before<br />
and after annealing recor<strong>de</strong>d using<br />
Brewster inci<strong>de</strong>nce. The inset in this gure<br />
shows an enlarged view of the <strong>Si</strong>-H<br />
peak variations with annealing.<br />
It can be seen that the LO 3 peak intensity<br />
gradually increases with increasing<br />
annealing temperatures. Consi<strong>de</strong>ring<br />
the eect of time, for a given temperature<br />
1000°C (1min-1000°C and 1h-<br />
1000°C) there is no signicant change in<br />
the LO 3 peak intensity whereas there is<br />
a drastic increase when the sample is annealed<br />
at 1h-1100°C.<br />
This trend represents a gradual evolution towards the phase separation process<br />
Figure 3.11: Eect of annealing on the<br />
FTIR spectra in Brewster inci<strong>de</strong>nce.<br />
upon annealing. A gaussian curve tting performed on these spectra indicated<br />
a reduction in the peak widths of LO 3 and TO 3 peaks with increasing annealing<br />
temperatures. Such reduction in the peak width with increasing annealing treatment<br />
has also been observed in [Morales-Sanchez 08] and these changes are attributed<br />
to the phase separation processes. In addition, we also notice an increase of the<br />
LO 4 −TO 4 mo<strong>de</strong> upon annealing. This indicates the disor<strong>de</strong>r in the matrix due to<br />
high <strong>Si</strong> excess. It can be seen that the <strong>Si</strong>-H peak appears only in the as-grown<br />
sample. The <strong>de</strong>sorption of hydrogen occurs with increasing annealing temperatures<br />
leading to a disappearance of this peak.<br />
(b) Raman spectroscopy<br />
The evolution of <strong>Si</strong>-np formation between as-grown and 1h-1100°C annealed SRSO-<br />
P15 sample as reected by FTIR spectra is conrmed through Raman spectroscopy<br />
following the procedure <strong>de</strong>tailed in chapter 2 un<strong>de</strong>r section 2.4.4 (Fig. 3.12).<br />
It can be seen that the as-grown sample shows a broad peak centered at 480<br />
cm −1 , which <strong>de</strong>creases in intensity after 1h-1100°C annealing with the appearance<br />
of a new peak at 517.6 cm −1 . The Raman spectrum of the as-grown layer shows<br />
dominant features of amorphous <strong>Si</strong>, since <strong>Si</strong>O 2 is reported to have a very low scattering<br />
cross section [Kanzawa 96, Khriachtchev 99]. This conrms the formation<br />
of amorphous <strong>Si</strong>-np in the as-grown sample as indicated by ∼24 at.% of agglomerated<br />
<strong>Si</strong> estimated using ellipsometry (Bruggeman) method (Ref. Tab. 3.6).<br />
76