X-Ray Fluorescence Analytical Techniques - CNSTN : Centre ...
X-Ray Fluorescence Analytical Techniques - CNSTN : Centre ...
X-Ray Fluorescence Analytical Techniques - CNSTN : Centre ...
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Figure IV.12a: Pulse height distribution<br />
(S) Gas proportional counter.<br />
Figure IV.12b: Pulse height distribution<br />
(Fe) Scintillation counter.<br />
If argon is used as the counting gas component in gas proportional counters, an<br />
additional peak, the escape peak (Figure IV.13), appears when X-ray energies are irradiated<br />
that are higher than the absorption edge of argon.<br />
Figure IV.13: Pulse height distribution (Fe) with escape peak.<br />
The escape peak arises as follows:<br />
The incident X-ray quant passes its energy to the counting gas thereby displaying a K electron<br />
from an argon atom. The Ar atom can now emit an Ar Kα1,2 X-ray quant with an energy of 3<br />
keV. If this Ar-fluorescence escapes from the counter then only the incident energy minus 3<br />
keV remains for the measured signal. A second peak, the escape peak that is always 3 keV<br />
below the incident energy, appears in the pulse height distribution.