Abstract

Neutron diffraction, 27Al MAS NMR, and 27Al Double Quantum MAS NMR results are presented and analyzed to determine the local environments of the cations in a series of aluminum tellurite glasses. Total scattering results show that, within a maximum Te–O distance of 2.36 Å, tellurium exhibits a mix of [TeO3E] and [TeO4E] environments (E = electron lone-pair), with a linear reduction in the average tellurium–oxygen coordination number as Al2O3 is added to the glass. This is accompanied by a linear decrease in the average aluminum–oxygen coordination number as [AlO4] units form at the expense of [AlO6] units, while the fraction of [AlO5] units remains roughly constant. A consideration of the bonding requirements of the five structural units in the glass, [TeO3E], [TeO4E], [AlO4], [AlO5], and [AlO6], has allowed a direct quantitative relationship between tellurium–oxygen and aluminum–oxygen coordination numbers to be derived for the first time, and this has been successfully extended to the boron tellurite system. Double Quantum 27Al MAS NMR indicates that, in contrast to previous reports, the shortest Al...Al separations are significantly smaller (∼3.2 Å) than expected for a uniform distribution and there is a preference for [AlO6]–[AlO6] and [AlO4]–[AlO4] corner sharing polyhedra. These associations support a new structural model which successfully applies the principle of charge balance to describe the interaction of tellurium and aluminum and identifies and explains the clustering of [AlOn] polyhedra in the glass and their preferred associations. [AlO6] and [TeO4E] units dominate the network in TeO2-rich glasses and [AlO4]− units form to stabilize the [TeO3E]+ units as alumina is added to the glass.

Highlights

  • Tellurite glasses have a range of superior functional properties, when compared to silica, which make them promising candidates for a range of optical applications in the near and mid infra-red (IR)

  • 4.1.1 Phase formation The synthesis conditions for the glasses used in this study were almost identical to those used by Kaur, Tagiara and Sakida

  • Similar separation has been observed in the boron tellurite glass system (> 20 mol% B2O3) which may provide a model for the immiscibility in the aluminium tellurite system.[44,45,46]

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Summary

Introduction

Tellurite glasses have a range of superior functional properties, when compared to silica, which make them promising candidates for a range of optical applications in the near and mid infra-red (IR) These properties include: higher refractive indices,[1] larger third-order non-linear optical coefficients,[2] lower phonon energies and extended transmittance into the infra-red.[1] In addition, tellurites can solubilise larger quantities of rare-earth (RE) ions than silicates without fluorescence quenching,[3] have good ionic conductivity and exhibit high dielectric constants.[1, 4,5,6] the exploitation of tellurite glasses is often limited by low melting points, poor durability and small regions of thermal stability. How these modifiers interact with the glass network, and each other, to give rise to the property changes is still poorly understood

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