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Determination of optimal metallic secondary target thickness, collimation, and exposure parameters for X‐ray tube‐based polarized EDXRF

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Tube‐based‐polarized energy‐dispersive X‐ray fluorescence (EDXRF) is a powerful adaptation on traditional EDXRF, requiring very specific geometry and a scattering target to generate polarized X‐rays. This secondary target is typically chosen to be a metallic foil, allowing for the polarization of the incident X‐ray beam, and the addition of the secondary target's fluorescence response to the initial beam. A simulation, using GEANT4 Monte Carlo code, and an experimental confirmation were used to determine the optimal thickness of a metallic secondary target for use in tube‐based‐polarized EDXRF. The optimal thickness was determined by looking at the signal‐to‐noise ratio (SNR). Using the results, the optimal thickness and tube potential were calculated for the common secondary target materials Cu, Mo, and Sn, when looking at an Fe sample. The optimal thickness results were compared with the results when using an ‘infinitely thick’ target. The results show improvements in SNRs of 6 − 17 % , illustrating the potential benefits of such calculations. Additionally, the optimal collimation of a polarized EDXRF system was examined, and it was found that increasing the total count rate should be the primary goal of geometrical optimization. If the count rate of the experimental setup is limited by tube output, then having the largest possible collimators yielded the maximum SNR. In contrast, if the count rate is limited by detector dead time, then decreasing the collimator size between secondary target and sample provided the maximal SNR. Copyright © 2017 John Wiley & Sons, Ltd.
Title: Determination of optimal metallic secondary target thickness, collimation, and exposure parameters for X‐ray tube‐based polarized EDXRF
Description:
Tube‐based‐polarized energy‐dispersive X‐ray fluorescence (EDXRF) is a powerful adaptation on traditional EDXRF, requiring very specific geometry and a scattering target to generate polarized X‐rays.
This secondary target is typically chosen to be a metallic foil, allowing for the polarization of the incident X‐ray beam, and the addition of the secondary target's fluorescence response to the initial beam.
A simulation, using GEANT4 Monte Carlo code, and an experimental confirmation were used to determine the optimal thickness of a metallic secondary target for use in tube‐based‐polarized EDXRF.
The optimal thickness was determined by looking at the signal‐to‐noise ratio (SNR).
Using the results, the optimal thickness and tube potential were calculated for the common secondary target materials Cu, Mo, and Sn, when looking at an Fe sample.
The optimal thickness results were compared with the results when using an ‘infinitely thick’ target.
The results show improvements in SNRs of 6 − 17 % , illustrating the potential benefits of such calculations.
Additionally, the optimal collimation of a polarized EDXRF system was examined, and it was found that increasing the total count rate should be the primary goal of geometrical optimization.
If the count rate of the experimental setup is limited by tube output, then having the largest possible collimators yielded the maximum SNR.
In contrast, if the count rate is limited by detector dead time, then decreasing the collimator size between secondary target and sample provided the maximal SNR.
Copyright © 2017 John Wiley & Sons, Ltd.

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