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Hi Soyoung,
I would not place too much importance to the value of the "Importance" factor ;) That is, it is a quick estimate of the importance of a Path so that it might be filtered out. As you'll notice, the first path always has an Importance factor of 100, making
comparisons between calculations difficult.
If you want to check how the scattering amplitude varies with angle, say to check how close it is to cosine-squared, I recommend reading in the Path files and integrating the magnitude of chi(k).
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Dear XAFS community,
I have a series of Ru K-edge data on a single-crystal RuO2 sample measured at different
incident X-ray angles. Because of the linear polarization of X-rays, the EXAFS of this single-crystal sample depends on the X-ray angle. I am trying to fit the four EXAFS spectra simultaneously with one set of parameters to extract the deltaR and MSRD parameters
of this sample.
For oriented samples, N for a certain single scattering path is supposed to be proportional
to 3*cos^2(θ), where θ is the angle btwn the X-ray's e-vector and the absorber-scatterer vector. Instead of manually calculating the 3cos^2(θ) for all of the scattering paths in RuO2 (there are 7 single and 3 multiple scattering paths that need to be included
to achieve a good fit with a reference RuO2 powder sample), I decided to use the polarization card in my FEFF input. For example, for one of the X-ray angles, the e-field vector would be (1, 0, 0), so I added the line "POLARIZATION 1 0 0" in the FEFF input
file.
Running this input file gave me a list of paths that had different importance values
for each path compared to the non-polarized (isotropic) calculation. Since "importance" is the relative magnitude of each path's scattering contribution (integration of the chi(k)), I thought that it would be proportional to 3cos^2(θ). That is, for
path i from a FEFF calculation for angle a, the "importance" (abbreviated as "Imp") of that path would be:
Imp(a)_i = C(a) * Imp(iso)_i * 3cos^2(θ_i)
where C(a) is a constant for each angle that accounts for the fact that importance
values are relative (because it is scaled so that the first path in the list has an importance of 100).
Now, I wanted to check whether the polarized FEFF calculations really follow this relationship
underlined above. So, I tried manually calculating the values of 3cos^2(θ) for two of the paths from the same polarized FEFF calculation, then plug them into the above equation to get C(a). But, as the table below shows, the C(a) values are not the same. FEFF
1 has a disagreement that is small enough to ignore, but the disgareement of C(a) values for The disagreement is small enough to ignore for FEFF 1, but for FEFF 2 and 3 the disagreements are quite large.
*FEFF 1, 2, 3 designate individual polarized FEFF calculations. FEFF 1 was with polarization
vector = (1, 0, 0). FEFF 2 and 3 were with polarization vector = (0.85, 1.13, 0). For this polarization, the two Ru sites gave different lists of paths.
I do think the qualitative trend of the "importance" values in the polarized FEFF calculations
is correct, and I can get a bad but not-disastrous fit from simultaneously fitting the data from different angles. However, the above analysis makes me wonder whether the "importance" values from polarized FEFF are truly proportional to 3cos^2(θ), and whether
my fitting models for different angles, which I derived from the polarized FEFF calculations, are correct. An alternative would be to manually calculate 3cos^2(θ) for all the paths, but I'm not sure how to calculate it for multiple scattering paths.
One note, I am running the FEFF calculation with Larix to get the importance values
(labeled as "amp ratio" in the list.dat file, in the FEFF output folder). I wonder if the default settings for getting these amp ratios are not accurate enough for my purposes. It would be nice if I could just pull out the 3cos^2(θ) terms from the FEFF calculations...
Anyways, thank you very much for reading this rather lengthy question. Hope it makes
sense, and I would appreciate any help regarding this.
Best,
Soyoung