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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 200<br />

Absorption coefficient / cm -1<br />

0.35<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

0.00<br />

4 3.8 3.6 3.4 3.2 3 2.8<br />

y0 0 ±0<br />

xc1 2953.27767 ±11.9114<br />

w1 416.06733 ±10.56243<br />

A1 94.81773 ±5.29757<br />

xc2 3223.55641 ±5.11007<br />

w2 276.96669 ±9.83858<br />

A2 56.6069 ±6.00553<br />

xc3 3384.02786 ±1.40624<br />

w3 144.54882 ±5.30864<br />

A3 16.02548 ±1.71867<br />

Baseline: y=[(1490/x)^4]+0.371<br />

Chi^2 = 0.00002<br />

R^2 = 0.99818<br />

Wavelength / µm<br />

FTIR data<br />

Gaussian fit<br />

Strong OH (2953 cm -1 )<br />

Weak OH (3224 cm -1 )<br />

Free OH (3384 cm -1 )<br />

2600 2800 3000 3200 3400 3600<br />

Wavenumber / cm -1<br />

Fig. (6.24): Gaussian deconvolution of the OH bands of glass MOD016 (70TeO2-<br />

25WO3-5Bi2O3 mol. %).<br />

Table (6.5) summarises the positions (P), half-widths (W), and areas (A) of these bands.<br />

Table (6.5): Positions (P), half-widths (W), and areas (A) of OH bands for glasses<br />

MOD014 (90TeO2-5WO3-5Nb2O5 mol. %), MOD015 (82.5TeO2-7.5WO3-10Nb2O5 mol.<br />

%), and MOD016 (70TeO2-25WO3-5Bi2O3 mol. %).<br />

Glass Strong OH Weak OH Free OH<br />

MOD P /<br />

ID cm -1<br />

W /<br />

cm -1<br />

A /<br />

(cm -1 ) 2<br />

P /<br />

cm -1<br />

W /<br />

cm -1<br />

A /<br />

(cm -1 ) 2<br />

P /<br />

cm -1<br />

W /<br />

cm -1<br />

A /<br />

(cm -1 ) 2<br />

014 2964 420 84.44 3213 247 31.97 3377 152 15.20<br />

015 2985 390 53.40 3239 249 26.38 3391 140 9.44<br />

016 2953 416 94.82 3224 277 56.61 3384 145 16.03<br />

Table (6.6) and fig. (6.25) summarise the areas of these bands.<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

Loss / dB.m -1

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