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Tellurite And Fluorotellurite Glasses For Active And Passive

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6. Optical properties; MDO 229<br />

a change in the multiphonon edge. Tellurium also has a higher charge than zinc, therefore<br />

also has a higher lattice energy. Using equation (2.8), addition of zinc will result in a<br />

decrease in µ (reduced mass), causing the edge to shift to higher frequencies.<br />

Fig. (6.13) shows the multiphonon edges of glass of composition 80TeO2-10Na2O-<br />

20ZnO mol. % (MOD013) with thickness viz. 2.98, 0.50 and 0.20 mm. The multiphonon<br />

edge was enhanced with decreasing thickness due to an increasing amount of signal<br />

reaching the detector. Ernsberger [14] has shown that by using very thin silicate glass<br />

samples it was possible to ‘extend the useful spectrum [of silicates] to ≈ 1,300cm -1 ’ i.e.<br />

enable us to see more clearly bands that were indistinguishable before. This is also true<br />

for tellurite glasses as fig. (6.14) and (6.15) show [5]. In the spectrum of thin (0.20 mm)<br />

glass, of composition 80TeO2.10ZnO.10Na2O (mol. %), the higher wavenumber shoulder<br />

of the 3060 cm -1 band can be more clearly discerned than in the spectra of the longer<br />

optical pathlength specimens (fig. (6.15)), and at least four bands thought to be related to<br />

structural units in the glass network (see below) can be seen within the multi-phonon<br />

absorption edge (fig. (6.14)). Fig. (6.16) to (6.17) show the Gaussian deconvolution of<br />

these OH bands in the longer optical pathlength samples.<br />

Scholze [17] identified a band around 3500 cm -1 for alkali metal silicate glasses and<br />

attributed this to the stretching mode of the free Si-OH groups. Ryskin [22, 23] also<br />

identified a band around 3500 cm -1 for hydrated crystalline silicates and attributed this to<br />

a stretching mode of the water molecule. It is therefore proposed that the band around<br />

3300 cm -1 in fig. (6.17) (which is a shoulder of the 3060 cm -1 band) be attributed to free<br />

Te-OH groups or molecular water (or a combination of both) [5]. By exposing thin glass<br />

films to a high a vapour pressure of water (i.e. steam) Ernsberger [14] entrapped

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