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CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

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eing bonded with the Si atoms (i.e. P-O-Si type of linkages). Phosphorus being more<br />

electronegative than Si, this will result in a reduction in the force constants, and hence<br />

lowering of Raman frequency. This effect is more prominent for the symmetric PO 4 vibration<br />

and hence we observe two peaks in the present case.<br />

Intensity (arb. units)<br />

(a)<br />

(b)<br />

(c)<br />

880 900 920 940 960<br />

Raman shift (cm -1 )<br />

Fig.71 Raman spectrum corresponding to symmetric PO 4 stretching mode of (a) un-doped<br />

3+<br />

3+ 3+<br />

SbPO4 (b) SbPO 4 :Ce (2.5%),Tb (5%) and (c) SbPO 4 :Ce (2.5%),Tb 3+ (5%) samples<br />

dispersed in silica.<br />

4.3.5 Luminescence studies on SbPO 4 :Ce, Tb and effect of incorporation of<br />

nanomaterials in silica: Figure 72 shows the emission spectra of SbPO :Tb 3+<br />

4 (5%),<br />

3+<br />

SbPO4:Ce (2.5%),Tb<br />

3+ 3+<br />

(5%) and SbPO 4 :Ce (2.5%),Tb 3+ (5%)-SiO 2 obtained after 250 nm<br />

excitation. The peaks observed ~ 489, 543, 585, and 621 nm correspond to transitions from<br />

5 D 4 level to 7 7 7 F 6, F 5, F 4 and 7 F levels, respectively of Tb 3+<br />

3 ion. It is worth noting that, unlike<br />

Tb 3+ or Ce 3+ -Tb 3+ doped SbPO 4 samples, pure TbPO4 prepared by the identical method as<br />

that of SbPO :Tb 3+<br />

4 samples did not show any emission (inset of Fig.72). This aspect<br />

substantiate the fact that Tb 3+ ions are getting incorporated in SbPO 4 lattice and do not exist<br />

as separate TbPO 4 phase, a fact which is also confirmed from the vibrational studies<br />

described above. It is also observed that Ce 3+ ion shows very weak emission in the UV<br />

3+ 3+<br />

region. A representative Ce emission spectrum from SbPO 4 :Ce (2.5%),Tb 3+ (5%) sample<br />

126

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