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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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6. Optical properties; MDO 191<br />

Absoprtion coefficient / cm -1<br />

120<br />

110<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

Wavelength / µm<br />

13 12 11 10 9 8 7 6<br />

MOD013: 80TeO 2 -10Na 2 O-10ZnO<br />

2.98 mm<br />

0.50 mm<br />

0.20 mm<br />

0<br />

750 1000 1250 1500 1750<br />

Wavenumber / cm -1<br />

Fig. (6.13): Infrared spectra in the mid- and far-infrared regions for glasses of<br />

composition MOD013 (80TeO2-10Na2O-10ZnO mol. %), performed on samples of<br />

thickness, 2.98, 0.50 and 0.20 mm.<br />

From fig. (6.13), it can be seen that the region where spectra were to be collected before<br />

the signal become too noisy (i.e. the detector was underloaded), was extended with<br />

decreasing thickness of the sample. <strong>For</strong> the 2.98 mm sample the spectra extended to<br />

around 1520 cm -1 (6.58 µm), for 0.50 mm to around 920 cm -1 (10.87 µm), and for 0.20<br />

mm to around 850 cm -1 (11.76 µm). Absorption bands within the multiphonon edge<br />

become more easily discernable with decreasing thickness of sample. Fig. (6.14), the<br />

bands seen in the multiphonon edge are seen for the 0.20 mm sample.

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