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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 226<br />

Absorption bands due to OH in glasses, and the solubility of water in glasses has been<br />

studied extensively in the literature [11-21]. Adams found that association of OH groups<br />

through hydrogen-bonding in silicate glasses produces three effects on infrared OH<br />

absorption bands [11]:<br />

1. decrease of the frequency of asymmetric stretching bands;<br />

2. enhancement of the integrated intensity and<br />

3. broadening of the contour of absorption bands.<br />

In general, multiple hydrogen-bonded OH absorption bands are found for silicate glasses<br />

only when modifiers (Na + , K + ) and / or intermediates (Ca 2+ , Pb 2+ ) are present, as the<br />

electronic structure of the oxygen atom changes, the field strength increases and the<br />

greater negative charge on the oxygen atom results in greater affinity for hydrolysis to<br />

occur [11]. Scholze [17] identified a number of vibrational absorption bands for silicate<br />

glasses which will be discussed in more detail later in this section, in relation to tellurite<br />

and fluorotellurite glasses. He found that vitreous silica possessed a single absorption<br />

band around 3675 cm -1 attributed to ‘free-OH’, which exhibits no hydrogen-bonding.<br />

Like Adams, Scholze found by adding alkali metal oxides such as Na2O that this band<br />

gradually shifted to longer wavelengths eventually overlapping with a band around 3000<br />

cm -1 not present in the spectrum of vitreous silica. This band, and another at around 2300<br />

cm -1 , was attributed to OH in the glass, which participates in hydrogen bonding of<br />

varying bond-strength and length [17]. Zarubin [19] has recently challenged this model<br />

by suggesting the bands around 3000, 2300 and a further band at 1800 cm -1 are the result

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