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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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2. Literature review; MDO 54<br />

be broader and flatter than for silicate based glasses (1530 to 1640 nm and 1520 to 1600<br />

nm respectively) [36].<br />

Feng et al. [54] showed that addition of GeO2 and Y2O3 to erbium (III) doped TeO2-<br />

GeO2-ZnO-Na2O-Y2O3 glasses, increased glass stability and the lifetime of 4 I13/2 level of<br />

the Er +3 ion.<br />

Shen et al. [55] showed that the replacement of ZnO and TeO2 with Na2O results in a<br />

narrowing of the emission band of erbium (III). The lifetime of erbium (III) in TeO2-<br />

Na2O-ZnO glasses reaches a maximum at 11000 ppmw Er +3 . Broadening of the 1.55 µm<br />

emission also occurs with increasing Er2O3 content. High OH content decreases the<br />

lifetimes of the 4 I13/2 4 I15/2 transition significantly [55]. Fibre drawn from this glass<br />

exhibited minimum loss of around 0.5 dB.m -1 at 1.3 µm, however, losses increases<br />

rapidly at lower and higher wavelengths. Fig. (2.13) shows the fibre loss spectra, with an<br />

inset of the theoretical intrinsic loss curve.<br />

Fig. (2.13): Loss spectra of Er +3 -doped TeO2-Na2O-ZnO fibre (inset shows theoretical<br />

intrinsic loss curve) [55].

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