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Films minces à base de Si nanostructuré pour des cellules ...

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

noticed that the intensity obtained after 4.75h-FG + STA is higher than that of<br />

100(3.5/5) STA ML (Fig. 4.42). This suggests that the time spent un<strong>de</strong>r 500 °C in<br />

4.75h-FG process in 50(3.5/5) has a similar eect of the 4.75h excess time spent by<br />

100(3.5/5) in the <strong>de</strong>position chamber.<br />

Figure 4.42: Investigating the PL spectra<br />

obtained from 50(3.5/5) SRSO/SRSN ML after<br />

FG+STA. (The PL spectra obtained after<br />

STA (1min-1000°C N 2 ) from 50 and 100 patterned<br />

MLs are also given in dotted lines for<br />

comparison).<br />

One possible reason could be the exodiusion<br />

of hydrogen at such high temperature<br />

(500°C) resulting in <strong>Si</strong> dangling<br />

bonds that reorganize to act as nucleating<br />

sites in the SRSO sublayers. Hence,<br />

a STA (1min-1000°C in N 2 ) treatment<br />

that follows after this time and temperature<br />

of exposure is sucient to result in<br />

a high <strong>de</strong>nsity of <strong>Si</strong>-np. Thus, we may<br />

say that the emission intensity increases<br />

with increasing <strong>de</strong>nsity of nanoclusters<br />

resulting in emission enhancement of 50<br />

patterned sample.<br />

These results indicate that the time<br />

spent at high temperature (500°C-either<br />

in <strong>de</strong>position chamber or in post fabrication<br />

process) prior to STA has a huge<br />

inuence in favouring emission. The dierent peak positions of 100(3.5/5) STA ML<br />

and 50(3.5/5) 4.75h+STA ML, can be attributed to the dierent annealing processes<br />

employed on these two MLs. Thus, these studies <strong>de</strong>monstrate the possibility of enhancing<br />

the emission of a SRSO/SRSN ML by reducing the material (50 patterns<br />

vs. 100 patterns) subjecting to a pre-thermal treatment before STA.<br />

4.10 Un<strong>de</strong>rstanding the origin of photoluminescence<br />

A <strong>de</strong>tailed investigation on various annealing treatment on the PL spectra in the<br />

previous sections suggested various possible origins for emission. It was seen in<br />

section 4.6 that mostly all the PL spectra obtained from samples annealed un<strong>de</strong>r<br />

N 2 atmosphere had three peaks. From the peak positions in all the investigations<br />

above, we might attribute a range of positions for these peaks named as (1,2,3) in<br />

100(3.5/5) ML and (a,b,c) in 50(3.5/5) ML. They are,<br />

- Peak (1) (a) and (b) :1.2-1.45 eV<br />

- Peak (2) and(c): 1.50-1.7 eV<br />

128

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