Hi Joe,
That's a fair point.
But there are really two types of APF corrections, one is what I call a "specified" APF and the other is what I call "compound" APFs. They are described in detail here:
https://probesoftware.com/smf/index.php?topic=536.0The "specified" APF is exactly as you describe, a perfectly matrix matched peak shift/shape factor that is applied when using a "specific" primary standard anjd a "specific"unknown. In this case, one is making a peak shift/shape correction factor for a specific unknown material, for a specific element and they need to be acquired and applied on a case by case basis. Usually as you say for quantifying a light element such as boron, nitrogen, oxygen or carbon. See Bastin's publications from the 90s on these:
https://probesoftware.com/smf/index.php?topic=1422.msg10470#msg10470See this white paper for an example of using "specified" APFs:
https://epmalab.uoregon.edu/reports/Preliminary%20work%20on%20MgB2%20and%20MgB4.pdfBut compound APFs are not matrix matched. They are created by combining single element APFs, which are grouped into families, for example oxides or carbides. One example for measuring oxygen one might use MgO as the primary standard for oxygen k-ratio and then combine fractions of the other oxides APFs (MgO to Al2O3, MgO to SiO2, MgO to Fe2O3, etc., etc.) that are present in the unknown to obtain a "compound" APF for your particular unknown composition. This calculation is performed in the matrix iteration in PFE.
These compound APFs are my own invention but they seem to work great and don't require performing a bunch of peak shape measurements, usually. See the Empirical APFs dialog in Probe for EPMA. Because the first order effect for chemical effects is the specific element chemical bonding, the secondary effect is valence (small effect) and the third order effect is coordination, which is usually an even weaker effect.
Yes, as you say, although one would think that these binary to compound APFs would vary from spectrometer to spectrometer, it's not as much of a problem as one might have thought. Partly I think because if one is (for example) measuring oxygen, you're probably using a W/Si LDE with a 2d around 60 angstroms which is what Bastin used (ignoring the stearate diffractors which due to their higher spectral resolution yield more larger APF effects than LDEs, but they are rarely if ever used these days). And again, for example nitrogen, we're all probably using an LDE specific for nitrogen. But of course this assumption should be tested.
Here is a test I did myself on MgO to Al2O3 and SiO2 and compared to Bastin's APF measurements:
https://epmalab.uoregon.edu/reports/APF%20measurements.docAnd yes, these peak shift/shape effects tend to become smaller with increasing emission line energy (it's basically a problem for emission lines that involve shells that are also involved in chemical bonding). And since we're talking at most a few percent APF corrections this only applies to major elements, not trace elements.
So for example we can in general ignore APF issues for Si ka by simply using a silicate standard as a primary standard, as opposed to using Si metal as a primary standard. If the Si atoms in the primary standard and unknown are both bonded to oxygen (e.g., SiO2 and Mg2SiO4), the chemical effects are very small and the APF issues can be ignored. The matrix correction can handle the physics.
The question is at what point can we use a metal as a primary standard for oxide materials. This is something discussed here:
https://probesoftware.com/smf/index.php?topic=1423.0