Author:
Donovan John J.,Tingle Tracy N.
Abstract
Quantitative EPMA (electron probe microanalysis) intensity
measurements require an accurate correction for the X-ray continuum
(or background) created by the Bremsstrahlung effect from the
primary electron beam. This X-ray continuum, as measured on
a wavelength-dispersive spectrometer at any particular wavelength,
is primarily a function of the mean atomic number of the material
being analyzed. One can calibrate the dependence of the continuum
on mean atomic number by measuring and curve fitting the X-ray
intensities at the analytical peak in pure elements, oxides,
and binary compound standards that do not contain any of the
analyte or any interfering elements and use that calibration
to calculate the X-ray background correction. For unknown samples,
the mean atomic number is determined from the elemental
concentrations calculated by the ZAF or φ(ρz) matrix
correction, and the fit regression coefficients are used
iteratively to calculate the actual background correction. Over
a large range of mean atomic number we find that the dependence
of the continuum intensity on mean atomic number is well described
by a second-order polynomial fit. In the case of low-energy
X-ray lines (<1 to 2 keV), this fit is significantly improved
by correcting the X-ray continuum intensities for absorption.
For major and most minor element analyses, the improved mean
atomic number background correction procedure presented in this
paper is accurate and robust for a wide variety of samples.
Empirical mean atomic number background data are presented for
a typical 10-element silicate and a 15-element sulfide analytical
set up that demonstrate the validity of the technique as well
as some potential limitations.
Publisher
Cambridge University Press (CUP)
Cited by
147 articles.
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