Tellurite And Fluorotellurite Glasses For Active And Passive
Tellurite And Fluorotellurite Glasses For Active And Passive Tellurite And Fluorotellurite Glasses For Active And Passive
2. Literature review; MDO 59 The glasses exhibited two absorption bands attributed to ‘water’, with maxima around 3.2 and 3.5 µm. Both bands are broad and overlap, but are of low intensity, and are practically non-existent in the glass with 51.81 mol. % ZnF2, due to chemical reactions which take place during melting as shown by equation (2.16) to (2.18). Nazabal et al. [30] showed a decrease in OH bands with increasing ZnF2 content in the glass as shown by fig. (2.15). Fig. (2.15): Infrared spectra of TeO2-ZnO-ZnF2 glasses [30]. It can be seen the OH bands were reduced by self-drying during melting as described by equations (2.16) to (2.18). Erbium (III) bands at around 1.55 µm in these glasses were shown to slightly broaden, and 4 I11/2 and 4 I13/2 lifetimes significantly increase (from 0.4 to 2.2 ms and 3 to 7 ms respectively, for 0 to 35 mol. % ZnF2) with fluorine content. This was though to be due to a combination of a change in ion-host field strengths, and reduction in OH content with fluorine addition [31].
2. Literature review; MDO 60 2.5.2.4. Mechanical properties Kumar et al. [59] studied the mechanical properties of TeO2-PbO-ZnF2 glasses, shown in table (2.8). Table (2.8): Mechanical properties of glasses (mol. %) A: 68TeO2-12PbO-20ZnF2, B: 59TeO2-11PbO-30ZnF2, C: 50TeO2-10PbO-40ZnF2, and D: 46TeO2-9PbO-45ZnF2 [59]. It can be seen, as the ZnF2 content was increased, and PbO decreased, the elastic coefficients of the glass increased. This was thought to be due to depolymerisation of the network with increasing PbO content, which the authors believe had a stronger effect than ZnF2 [59]. 2.6. References [1] H. Rawson, Inorganic glass-forming systems, vol. 2, 1st ed. London: Academic Press, 1967. [2] W. Vogel, Glass chemistry, 2nd ed. New York: Springer-Verlag, 1994. [3] J. T. Randall, H. P. Rooksby, and B. S. Cooper, Journal of the Society of Glass Technology, vol. 14, pp. 219-229, 1930. [4] B. E. Warren, Journal of Applied Physics, vol. 8, pp. 645-654, 1937.
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2. Literature review; MDO 59<br />
The glasses exhibited two absorption bands attributed to ‘water’, with maxima around 3.2<br />
and 3.5 µm. Both bands are broad and overlap, but are of low intensity, and are<br />
practically non-existent in the glass with 51.81 mol. % ZnF2, due to chemical reactions<br />
which take place during melting as shown by equation (2.16) to (2.18).<br />
Nazabal et al. [30] showed a decrease in OH bands with increasing ZnF2 content in the<br />
glass as shown by fig. (2.15).<br />
Fig. (2.15): Infrared spectra of TeO2-ZnO-ZnF2 glasses [30].<br />
It can be seen the OH bands were reduced by self-drying during melting as described by<br />
equations (2.16) to (2.18). Erbium (III) bands at around 1.55 µm in these glasses were<br />
shown to slightly broaden, and 4 I11/2 and 4 I13/2 lifetimes significantly increase (from 0.4 to<br />
2.2 ms and 3 to 7 ms respectively, for 0 to 35 mol. % ZnF2) with fluorine content. This<br />
was though to be due to a combination of a change in ion-host field strengths, and<br />
reduction in OH content with fluorine addition [31].