Article contents
A Model for Characteristic X-Ray Emission in Electron Probe Microanalysis Based on the (Filtered) Spherical Harmonic (
$P_{\rm N}$) Method for Electron Transport
Published online by Cambridge University Press: 11 April 2022
Abstract
Classical $k$-ratio models, for example, ZAF and
$\phi ( \rho z)$, used in electron probe microanalysis (EPMA) assume a homogeneous or multilayered material structure, which essentially limits the spatial resolution of EPMA to the size of the interaction volume where characteristic X-rays are produced. We present a new model for characteristic X-ray emission that avoids assumptions on the material structure to not restrict the resolution of EPMA a priori. Our model bases on the spherical harmonic (
$P_{\rm N}$) approximation of the Boltzmann equation for electron transport in continuous slowing down approximation.
$P_{\rm N}$ models have a simple structure, are hierarchical in accuracy and well-suited for efficient adjoint-based gradient computation, which makes our model a promising alternative to classical models in terms of improving the resolution of EPMA in the future. We present results of various test cases including a comparison of the
$P_{\rm N}$ model to a minimum entropy moment model as well as Monte-Carlo (MC) trajectory sampling, a comparison of
$P_{\rm N}$-based
$k$-ratios to
$k$-ratios obtained with MC, a comparison with experimental data of electron backscattering yields as well as a comparison of
$P_{\rm N}$ and MC based on characteristic X-ray generation in a three-dimensional material probe with fine structures.
Keywords
- Type
- Software and Instrumentation
- Information
- Copyright
- Copyright © The Author(s), 2022. Published by Cambridge University Press on behalf of the Microscopy Society of America
References
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline367.png?pub-status=live)
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline368.png?pub-status=live)
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline369.png?pub-status=live)
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline370.png?pub-status=live)
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline371.png?pub-status=live)
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20221109172053821-0608:S1431927622000083:S1431927622000083_inline372.png?pub-status=live)
- 3
- Cited by