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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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7. Surface properties; MDO 310<br />

binding energy [19]. Intermediates in the glass such as Zn +2 can also result in termination<br />

of the glass network in places, much like Na + , but weakly link it in others [21]. Therefore,<br />

the main O1s peak at around 530.9 eV (82.5 %) eV is a combination of the binding<br />

energies of oxygens within BOs and NBOs in the glass.<br />

The spectrum from the polished surface of glass MOD015 (fig. (7.10)) clearly shows<br />

that the O1s peak attributed to OH at 532.4 eV (46.3 %) has clearly grown, due to<br />

hydrolysis at the exposed glass surface, in addition to the main peak at 530.6 eV (46.5<br />

%). An additional peak can be seen at 533.9 eV (7.2 %), most likely to be due to organic<br />

groups (C-O / C=O) at the glass surface.<br />

7.3.1.3. XPS of fluorotellurite glasses<br />

No XPS studies, to this author’s knowledge, have been performed on fluorotellurite<br />

glasses. However, Chowdari et al. performed XPS studies on CuI containing TeO2<br />

glasses [20].<br />

Fig. (7.11) shows the wide scan XPS spectra of glass MOF001_iii (65TeO2-10Na2O-<br />

25ZnF2 mol. %), which was melted for 1.75 hours with un-fluorinated ZnF2. Na1s, Zn2p,<br />

F1s, Te3d, and O1s peaks were identified and quantification is shown. Quantification<br />

from the wide scan gives a rough estimate of composition, however the high resolution<br />

peaks give more accurate values. The F1s peak (fig. (7.12)) was asymmetric, the higher<br />

energy shoulder at 684.4 eV now almost a separate peak of similar area to the peak at<br />

681.9 eV (51.0 and 49.0 % respectively). This multipeak structure is to be expected, as<br />

although fluorine enters the glass in ZnF2, it will probably bond to other cations in the

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