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CHEM01200604004 Shri Sanyasinaidu Boddu - Homi Bhabha ...

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peak can be attributed to the crystal field effect on the Er 3+ energy levels. Excitation spectrum<br />

corresponding to 1536 nm emission of Er 3+ ions is shown in Fig.116 (b). It is consist of broad<br />

peak at 255 nm along with sharp peaks at 380, 488 and 522 nm. The broad band is due to the<br />

charge transfer process in WO 2- 4 structural units and sharp peaks are due to f-f transitions of<br />

Er 3+ ion in the CaWO 4 lattice. The appearance of 255 nm band in the excitation spectrum<br />

corresponding to Er 3+ emission indicates that energy transfer is taking place from host to Er 3+<br />

ions.<br />

Intensity (arb.units)<br />

250000<br />

200000<br />

150000<br />

100000<br />

50000<br />

λ exc<br />

255 nm<br />

380 nm<br />

522 nm<br />

0<br />

1400 1450 1500 1550 1600 1650<br />

Wavelength (nm)<br />

(a)<br />

Intensity (arb.units)<br />

14000<br />

λ<br />

12000<br />

em<br />

= 1536 nm<br />

10000<br />

8000<br />

6000<br />

4000<br />

2000<br />

0<br />

250 300 350 400 450 500 550 600<br />

Wavelength (nm)<br />

(b)<br />

Fig.116. (a) Emission spectrum and (b) excitation spectrum of Er 3+ doped CaWO 4<br />

nanoparticles.<br />

179

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