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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2. Possible formation of Si-O-N bonds at the interface of SRSO and SRSN sublayers. 3. It has been reported in SiN x monolayers that the presence of nitrogen atoms as the next nearest neighbours would induce a shift of the TO mode towards higher wavenumbers [Molinari 03]. The same proposition can be assumed in the case of SRSO/SRSN MLs. tel-00916300, version 1 - 10 Dec 2013 In addition to these peaks, it also has to be remembered that the (LO 4 -TO 4 ) Si−O modes may also contribute to the shape and peak positions of the FTIR spectra. Similarly the normal incidence spectrum also shows the contribution of Si-O from SRSO and Si-N from SRSN layers (Fig. 4.19b) and is tted with four peaks. The two major peaks centered around 1058 cm −1 and 887 cm −1 can be unambiguously attributed to the (TO 3 ) Si−O and TO Si−N modes respectively. Figure 4.20: FTIR spectra of as-grown and CA 100(3.5/5) ML. The presence of Si excess in SRSO sublayer is attested by the shift of the (TO 3 ) Si−O peak position towards lower wavenumbers as compared to that in SiO 2 (∼1080 cm −1 ). The less intense peaks around 1186 cm −1 and 806 cm −1 can be attributed to the TO 4 and TO 2 modes of Si-O respectively. Figure 4.20 shows the the FTIR spectra of as-grown and CA 100(3.5/5) ML recorded in Brewster and normal incidences. The position and intensity of the FTIR bands is a result of an overlapping contribution from Si-O and Si-N modes thereby making the analysis complicated. Hence the identication of the peaks are very dicult after annealing and the tting of peaks are therefore not appropriate. The approximate peak positions of the dierent vibration modes are indicated on the top part of the gure. From a comparison of the overall shape of the spectra obtained from the as-grown and CA samples, it can be seen that the Brewtser incidence spectra show a blueshift (towards higher wavenumber) of the peak maximas. The blueshift of the Si-O modes with annealing is indicative of the formation of Si-np in SRSO sublayer. This is conrmed by the increase of (LO 3 ) Si−O mode 110

around 1250 cm −1 . The blueshift of the Si-N modes is evident from FTIR spectra recorded in both angle of incidences and can be ascribed to the evolution of SRSN sublayer towards Si 3 N 4 . Similar shifts have been observed in SiN x monolayers when annealed at 950°C for t A > 1h under nitrogen atmosphere [Molinari 03]. 4.5.4 Surface Microstructure tel-00916300, version 1 - 10 Dec 2013 Preliminary surface microstructural investigations were performed using optical microscopy on the as-grown and CA 100(3.5/5) ML (Fig. 4.21). The surface of the as-grown sample is completely smooth whereas the surface of the CA sample shows appearance of circular spots of varying diameters ranging between less than 1 µm to about 200 µm. The possible reasons for appearance of these circular spots can be attributed to the reactive growth process leading to gas (N,H) exodiusion Figure 4.21: Surface microstructure of upon annealing. Consequently, the annealing procedure will be a key point for 100(3.5/5) ML. as-grown and 1h-1100°C annealed (CA) the achievement of a suitable lm. 4.5.5 X-Ray Diraction XRD analyses were performed on the as grown and CA samples (Fig. 4.22). The broad peak in the range between 20-30° seen in the as-grown sample relates to the presence of amorphous Sinp. The XRD spectrum of the CA sample exhibits a sharper peak around 28° referring to the Si (111) plane that can be tted with a single gaussian peak conrming the presence of Si nanocrystals. The high intensity of (111) peak and the clear presence of (220) peak which is not often witnessed, suggest a high density of Si-np formed in the SRSO and/or SRSN sublayers. Using Scherrer formula, the approximate Si-np size in the Figure 4.22: XRD spectra of asgrown and CA 100(3.5/5) ML. 111

2. Possible formation of <strong>Si</strong>-O-N bonds at the interface of SRSO and SRSN<br />

sublayers.<br />

3. It has been reported in <strong>Si</strong>N x monolayers that the presence of nitrogen atoms<br />

as the next nearest neighbours would induce a shift of the TO mo<strong>de</strong> towards higher<br />

wavenumbers [Molinari 03]. The same proposition can be assumed in the case of<br />

SRSO/SRSN MLs.<br />

tel-00916300, version 1 - 10 Dec 2013<br />

In addition to these peaks, it also has to be remembered that the (LO 4 -TO 4 ) <strong>Si</strong>−O<br />

mo<strong>de</strong>s may also contribute to the shape and peak positions of the FTIR spectra.<br />

<strong>Si</strong>milarly the normal inci<strong>de</strong>nce spectrum also shows the contribution of <strong>Si</strong>-O from<br />

SRSO and <strong>Si</strong>-N from SRSN layers (Fig. 4.19b) and is tted with four peaks. The<br />

two major peaks centered around 1058 cm −1 and 887 cm −1 can be unambiguously<br />

attributed to the (TO 3 ) <strong>Si</strong>−O and TO <strong>Si</strong>−N mo<strong>de</strong>s respectively.<br />

Figure 4.20: FTIR spectra of as-grown and CA<br />

100(3.5/5) ML.<br />

The presence of <strong>Si</strong> excess<br />

in SRSO sublayer is attested<br />

by the shift of the (TO 3 ) <strong>Si</strong>−O<br />

peak position towards lower<br />

wavenumbers as compared to<br />

that in <strong>Si</strong>O 2 (∼1080 cm −1 ).<br />

The less intense peaks around<br />

1186 cm −1 and 806 cm −1 can be<br />

attributed to the TO 4 and TO 2<br />

mo<strong>de</strong>s of <strong>Si</strong>-O respectively.<br />

Figure 4.20 shows the the<br />

FTIR spectra of as-grown and<br />

CA 100(3.5/5) ML recor<strong>de</strong>d<br />

in Brewster and normal inci<strong>de</strong>nces.<br />

The position and intensity<br />

of the FTIR bands is a result<br />

of an overlapping contribution from <strong>Si</strong>-O and <strong>Si</strong>-N mo<strong>de</strong>s thereby making the<br />

analysis complicated. Hence the i<strong>de</strong>ntication of the peaks are very dicult after<br />

annealing and the tting of peaks are therefore not appropriate. The approximate<br />

peak positions of the dierent vibration mo<strong>de</strong>s are indicated on the top part of the<br />

gure. From a comparison of the overall shape of the spectra obtained from the<br />

as-grown and CA samples, it can be seen that the Brewtser inci<strong>de</strong>nce spectra show<br />

a blueshift (towards higher wavenumber) of the peak maximas.<br />

The blueshift of the <strong>Si</strong>-O mo<strong>de</strong>s with annealing is indicative of the formation<br />

of <strong>Si</strong>-np in SRSO sublayer. This is conrmed by the increase of (LO 3 ) <strong>Si</strong>−O mo<strong>de</strong><br />

110

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