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tion but within a dierence of one or<strong>de</strong>r of magnitu<strong>de</strong>. It can also be seen that at<br />

high energies, the level of absorption in SRSO/SRSN ML approaches that of <strong>Si</strong>. This<br />

shows that the replacement of <strong>Si</strong>O 2 by SRSN sublayers in ML favours absorption.<br />

Despite a higher pump absorption in CA SRSO/SRSN ML, in comparison to<br />

SRSO/<strong>Si</strong>O 2 ML, there is a quenching of PL from the former. This implies that CA<br />

SRSO/SRSN ML favours absorption but has a <strong>de</strong>trimental eect on emission.<br />

4.6 Eect of annealing treatment un<strong>de</strong>r N 2 ow<br />

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

It was seen in the previous sections that the SRSO/SRSN samples contain nanocrystals<br />

as SRSO/<strong>Si</strong>O 2 MLs, but the presence of SRSN sublayers create a <strong>de</strong>trimental<br />

eect on the PL emission after CA. However, both the as grown (not shown) and<br />

CA SRSO/SRSN MLs have high α values. These results indicate the possibility of<br />

intermediate annealing treatments that might favour PL emission. A <strong>de</strong>tailed investigation<br />

on the eect of annealing treatments (temperature and time) was ma<strong>de</strong><br />

to optimize the PL emission.<br />

Annealing steps<br />

1min<br />

1+15min<br />

1+15+15min<br />

1+15+15+30min<br />

1h continuous annealing<br />

Denoted as<br />

1min (1min<br />

1000°C-STA)<br />

16min<br />

31min<br />

61min<br />

LTA<br />

(1h-1100°C-CA)<br />

Figure 4.27: Pictorial representation of step by step annealing un<strong>de</strong>r N 2 ow. (Table)<br />

Details of annealing time used for investigation and their notations.<br />

The 100(3.5/5) ML was annealed at various temperatures (T A ) between 400°-<br />

1100°C while the time of annealing (t A ) was varied between 1 minute to 61 minutes<br />

in steps as can be seen in the pictorial representation of gure 4.27. Continuous<br />

Long Time Annealing (LTA) of 1 hour at various temperatures were also performed.<br />

The emission obtained from LTA MLs were compared with MLs annealed for 61<br />

minutes in steps. Table of gure 4.27 <strong>de</strong>tails the various annealing steps employed<br />

for these investigations and the way they are <strong>de</strong>noted in the forthcoming parts. The<br />

eect of T A and t A on the emission intensities of SRSO/SRSN ML are discussed<br />

below. (All the graphs in the discussions that follow in this section are comparable).<br />

115

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