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Tellurite And Fluorotellurite Glasses For Active And Passive

Tellurite And Fluorotellurite Glasses For Active And Passive

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7. Surface properties; MDO 256<br />

where σ is the photoelectric cross-section, ζ the fraction of photoelectric events which<br />

take place without intrinsic plasmon excitation, λ the mean free-path in the sample, η the<br />

kinetic energy dependent spectrometer transmission, and I the area of the peak [3]. Cross-<br />

sections are well known from theoretical calculations by Scofield [4], the mean free path<br />

can be estimated from a universal curve, which depends on the energy of the incident<br />

beam, not the atomic number of the sample, and η is inversely proportional to the kinetic<br />

energy. Due to the superimposition of intrinsic and extrinsic plasmon events, ζ is difficult<br />

to estimate. Often the entire loss tail is assigned to extrinsic events, i.e. ζ = 1. This can<br />

introduce in significant errors into quantification, as ζ is not necessarily the same for two<br />

individual elements in a compound [3].<br />

7.1.2. Chemical and environmental durability<br />

7.1.2.1. Method<br />

<strong>For</strong> the chemical durability etching studies glass samples (of dimensions 3 × 5 × 5 mm,<br />

polished as described in section 6.1.1.1.) were immersed in a solution of 50 ml of the<br />

etchant, in a Pyrex beaker (250 ml capacity). <strong>For</strong> samples etched at 15 or 21°C, the<br />

beaker containing the etchant was surrounded by a constant temperature water bath, and<br />

the experiment begun (i.e. the sample was immersed) when the etchant had reached the<br />

appropriate temperature, measured with a mercury thermometer. <strong>For</strong> some samples<br />

(where stated) these were removed from the water bath to a sonic bath and agitated<br />

ultrasonically at room temperature (measured), to ensure homogeneous etching on all

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