CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...
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vibration of the Sb 4 O 6 ring is decomposed into 2A 1 + 2E + 2T 1 + 4T 2 of which A 1 , E and T 2<br />
are Raman active modes. These modes are further classified into Sb–O–Sb stretch, Sb–O–Sb<br />
bend and Sb–O–Sb wag modes [210]. The most affected modes in the nanorods (compared to<br />
bulk Sb 2 O 3 ) are the Sb–O–Sb stretching (A 1 type) appearing at ~256 cm -1 and the Sb–O–Sb<br />
bending (A 1 type) appearing at ~ 445 cm -1 . Another peak at ~ 710 cm -1 , also corresponds to<br />
Sb–O–Sb stretching with T 2 symmetry. As reported above, the shape selective nature of the<br />
nanorods results in only few of the modes that are affected, rest being unaltered. In<br />
comparison to the bulk material, the oriented Sb 2 O 3 nanorods are expected to have Raman<br />
activity in terms of the dynamic polarizability tensor. The A 1 type of vibrations include<br />
polarizability of the kind α xx + α yy + α zz , while T 2 type of vibrations includes the non-diagonal<br />
components like α xy , α yz , α zx [211]. Thus, the arrangement of the Sb 4 O 6 molecular units in<br />
Sb 2 O 3 nanorods is associated with the selective excitation of some of these polarizability<br />
tensors over the others, leading to enhanced Raman activity for a particular peak over the<br />
other. This results in appearance of additional peak at ~ 256 cm -1 and a triplet at ~ 445 cm -1<br />
for oriented samples. The A 1 type of modes have highest Raman activity (16 Å 4 amu -1 ) as<br />
compared to E, T 1 and T 2 type [210]. Moreover, these shape selective changes in the dynamic<br />
polarizability tensor is further regained to its bulk value (or at least tries to regain) by<br />
annealing the nanorods at 100 and 200°C. Thus, the Raman and XRD investigations suggest<br />
a clear morphological change in the Sb 2 O 3 , from nanorods to bulk particles. The structural<br />
changes associated with morphological change are responsible for the change in<br />
luminescence properties.<br />
In the following section brief description regarding the interaction of these<br />
luminescent nanorods with lanthanide ions are discussed. Eu 3+ ions are used as representative<br />
lanthanide ions in the present study as its luminescence properties with respect to different<br />
environments are well understood.<br />
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