CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
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On annealing the nanorods at 100 and 200°C, emission intensity of the 545 and 592<br />
nm peaks relative to the band edge emission has been found to decrease as can be seen from<br />
Fig.44 (c). Based on the luminescence and XRD studies of the as prepared nanorods and the<br />
nanorods annealed at different temperatures it is inferred that the morphological changes are<br />
taking place in Sb 2 O 3 nanorods during annealing and they are responsible for the change in<br />
intensity of 545 and 592 nm peaks. To further confirm the morphological assisted changes<br />
and the associated structural changes in Sb 2 O 3 nanorods on annealing, Raman spectroscopic<br />
studies of both (as prepared and annealed) samples were carried out and the results are<br />
described below. Figure 45 (a) shows Raman spectrum of the as prepared nanorods. The<br />
sample shows peaks at 143, 191, 218, 256, 297, 445, 503, 596 and 681 cm -1 , characteristic of<br />
the orthorhombic valentinite form of Sb 2 O 3 , which agrees well with the reported by data [64,<br />
207–209]. Similar spectra are also observed from bulk and nanorods annealed at different<br />
temperatures. The Raman spectra of the annealed samples show a strong luminescence<br />
background, intensity of which systematically increases as the annealing temperature is<br />
increased. Thus, the broad emission background dominates the sample annealed at 400°C.<br />
The major differences between the patterns corresponding to as prepared nanorods, the one<br />
annealed at different temperatures and the bulk, are depicted by the Raman peaks at ~260 cm -<br />
1 (Fig.45 (b)), 445 cm -1 (Fig.45 (c)) and ~ 710 cm -1 (Fig.45 (d)). The peak at ~ 260 cm -1 (peak<br />
A) in bulk Sb 2 O 3 is clearly seen to have evolved into two peaks for nanorods; one at 256 cm -1<br />
(peak A1) and another at 259 cm -1 (peak A2). The peak A1 is relatively sharper (line width<br />
approximately ~1/3 rd ) than peak A2. As the nanorods are annealed, the intensity of this peak<br />
reduces and that of A2 increases; while their widths remain almost constant. Similar<br />
inferences are drawn for the peak at ~ 445 cm -1 (peak B in Fig.45 (c)). In case of nanorod<br />
sample this shows a triplet, with peaks at ~ 435 cm -1 (peak B1), 443 cm -1 (peak B2) and 451<br />
cm -1 peak (B3). The B2 peak is most intense, followed by B3 and B1. The widths of peak B2<br />
90