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EXAFS as a tool for catalyst characterization: a review of the ... - INT

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Figure 3: Fourier trans<strong>for</strong>m corresponding to <strong>EXAFS</strong> spectrum <strong>of</strong><br />

metallic cobalt.<br />

When <strong>the</strong> contribution <strong>of</strong> two shells is not resolved in <strong>the</strong> Fourier<br />

spectrum, Fourier filtering can be used. By means <strong>of</strong> a filter function,<br />

specific peaks in <strong>the</strong> Fourier spectrum are separated from <strong>the</strong> rest <strong>of</strong><br />

<strong>the</strong> spectrum. The product <strong>of</strong> <strong>the</strong> spectrum with this filter function is<br />

Fourier backtrans<strong>for</strong>med into k space. This procedure separates <strong>the</strong><br />

contribution <strong>of</strong> adjacent coordination shells so that <strong>the</strong> effect <strong>of</strong> only<br />

<strong>the</strong> coordination shell <strong>of</strong> interest is maintained.<br />

In fact, <strong>the</strong> Fourier backtrans<strong>for</strong>m is calculated by<br />

(13)<br />

where W(κ) is <strong>the</strong> window <strong>of</strong> <strong>the</strong> Fourier trans<strong>for</strong>m and W’(κ) is <strong>the</strong><br />

window <strong>of</strong> <strong>the</strong> Fourier backtrans<strong>for</strong>m which separate <strong>the</strong> specific<br />

peak.

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