Tellurite And Fluorotellurite Glasses For Active And Passive
Tellurite And Fluorotellurite Glasses For Active And Passive Tellurite And Fluorotellurite Glasses For Active And Passive
% OH 100 90 80 70 60 50 40 30 20 10 0 6. Optical properties; MDO 215 0.0 0.2 0.4 0.6 0.8 1.0 ZnO / ZnF2 ratio Strong OH Weak OH Free OH Fig. (6.43): Percentage of OH groups for glasses of the series 65TeO2-(25-x)ZnF2-xZnO- 10Na2O mol. %, for 5 ≤ x ≤ 25 mol. % (MOF009 to 013). Table (6.10): Percentage of OH groups for glasses of the series 65TeO2-(25-x)ZnF2xZnO-10Na2O mol. %, for 5 ≤ x ≤ 25 mol. % (MOF009 to 013). Glass ZnO / ZnF2 Strong Weak Free MOF ID ratio OH / % OH / % OH / % 001 0.0 - 71 29 009 0.2 - 75 25 010 0.4 - 76 24 011 0.6 - 72 28 012 0.8 - 75 25 013 1.0 25 50 25
6. Optical properties; MDO 216 6.2.1.3. Spectroscopy of Er +3 -doped composition When a glass host which transmits in the NIR region is doped with erbium, emission bands are seen in this region (around 1.5 µm) due to the large number of energy levels of the Er +3 ion (such as 4 I15/2 4 I13/2). This phenomenon can be used to amplify signals carried by the glass in this important telecommunications window. Doping of fluorotellurite glass compositions was investigated here. The glasses were heat treated to investigate possible modification of the erbium bands with time and temperature. Fig. (6.44) shows the near-IR spectra of glass MOF017 (69.86TeO2-9.98Na2O- 19.96ZnF2-0.20ErF3 mol. %) as-annealed, and heat treated for 1 hour at 245, 255, 265 and 275°C. Absoprtion coefficient / cm -1 0.11 0.10 0.09 0.08 0.07 0.06 0.05 0.04 0.03 0.02 0.01 0.00 Wavelength / µm 1.60 1.55 1.50 1.45 6200 6400 6600 6800 7000 Wavenumber / cm -1 Untreated 1 hr. 245 o C 1 hr. 255 o C 1 hr. 265 o C 1 hr. 275 o C Fig. (6.44): Near-IR spectra of glass MOF017 (69.86TeO2-9.98Na2O-19.96ZnF2- 0.20ErF3 mol. %) untreated, and heat treated for 1 hour at 245, 255, 265 and 275°C. 110 100 90 80 70 60 50 40 30 20 10 0 Loss / dB.m -1
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6. Optical properties; MDO 216<br />
6.2.1.3. Spectroscopy of Er +3 -doped composition<br />
When a glass host which transmits in the NIR region is doped with erbium, emission<br />
bands are seen in this region (around 1.5 µm) due to the large number of energy levels of<br />
the Er +3 ion (such as 4 I15/2 4 I13/2). This phenomenon can be used to amplify signals<br />
carried by the glass in this important telecommunications window. Doping of<br />
fluorotellurite glass compositions was investigated here. The glasses were heat treated to<br />
investigate possible modification of the erbium bands with time and temperature.<br />
Fig. (6.44) shows the near-IR spectra of glass MOF017 (69.86TeO2-9.98Na2O-<br />
19.96ZnF2-0.20ErF3 mol. %) as-annealed, and heat treated for 1 hour at 245, 255, 265<br />
and 275°C.<br />
Absoprtion coefficient / cm -1<br />
0.11<br />
0.10<br />
0.09<br />
0.08<br />
0.07<br />
0.06<br />
0.05<br />
0.04<br />
0.03<br />
0.02<br />
0.01<br />
0.00<br />
Wavelength / µm<br />
1.60 1.55 1.50 1.45<br />
6200 6400 6600 6800 7000<br />
Wavenumber / cm -1<br />
Untreated<br />
1 hr. 245 o C<br />
1 hr. 255 o C<br />
1 hr. 265 o C<br />
1 hr. 275 o C<br />
Fig. (6.44): Near-IR spectra of glass MOF017 (69.86TeO2-9.98Na2O-19.96ZnF2-<br />
0.20ErF3 mol. %) untreated, and heat treated for 1 hour at 245, 255, 265 and 275°C.<br />
110<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
0<br />
Loss / dB.m -1