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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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1. Introduction; MDO 4<br />

Infrared transmission is useful for spectroscopic sensing of chemicals / organic<br />

groups, whose fundamental absorption bands occur in the mid-IR region. Bandwidth, and<br />

hence information carrying capacity is maximaised at zero dispersion (d 2 n/dλ 2 =0,<br />

occurring at 1.3 µm for silica, and at longer wavelengths for infrared transmitting<br />

materials), and intrinsic scattering losses fall with increasing wavelength [10].<br />

A high linear refractive index generally results in higher non-linearity than silica, with<br />

the possibility for use in high-speed switching and high power delivery devices. <strong>Glasses</strong><br />

with an induced second-order non-linearity can be used for second harmonic generation.<br />

The third-order non-linearity can be utilised in devices to boost the transmitted signal<br />

with solitons, and the bandwidth increased with all-optical processing [12]. Raman<br />

amplification is another way of amplifying the signal carried by the fibre, and is an<br />

intrinsic non-linear property of the material. Novel glasses have been shown to exhibit<br />

Raman gain much higher than silica [13].<br />

1.3. Aims and objectives of this study<br />

The glasses studied here, tellurite and fluorotellurite (TeO2-based), exhibit many of the<br />

desirable properties listed in section 1.2, and therefore show potential in a number of<br />

devices and applications. However, there is not much published work to date, particularly<br />

on fluorotellurite glasses. Useful properties include transmission from the visible (400<br />

nm) to the mid-IR (6 µm) [11], high refractive index (≈ 2, compared to ≈ 1.5 of silica<br />

[14]), large non-linearity (non-linear refractive index two orders of magnitude greater<br />

than silica [12]), with broad, long erbium (III) lifetimes [15], and Raman gain around 30

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