Rmax is not the problem here. This is a CIF file that the software is not interpreting correctly for some reason. I am quite sure that the Re-O near neighbor distance in NaReO4 is NOT 1.1191 AA. That -- not the error message -- should have been the thing you asked about! The CIF file is calling for I 41/a (group 88) origin choice #2. I would guess that Demeter is not interpreting the origin correctly. I'll put this on my to do list, but I have not been able to spend much time on Demeter in recent months. You might need to use something that is smarter about crystallography data than my software -- Crystal Maker or whatnot -- and make a feff.inp file by hand. B On 08/15/2018 09:42 AM, Dien.Li@srnl.doe.gov wrote:

Hi, Carlo and Matt or others

Attached please find the cif crystal structure data file for NaReO4 that was downloaded from Crystallography Open database. As I added it into Artemis for calculation, it gave error message saying that it has more than 500 atoms that exceeds the limit. Could you help to troubleshooting?? Thanks a lot.

Dien Li

-----Original Message----- From: Ifeffit On Behalf Of ifeffit-request@millenia.cars.aps.anl.gov Sent: Tuesday, August 14, 2018 5:29 PM To: ifeffit@millenia.cars.aps.anl.gov Subject: Ifeffit Digest, Vol 186, Issue 13

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Today's Topics:

1. Re: LCF on Larch - EXAFS Region (Matt Newville) 2. Re: wavelet transforms for EXAFS (Matt Newville)

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Message: 1 Date: Tue, 14 Aug 2018 12:33:35 -0500 From: Matt Newville To: XAFS Analysis using Ifeffit Subject: Re: [Ifeffit] LCF on Larch - EXAFS Region Message-ID: Content-Type: text/plain; charset="utf-8"

Hi Martin and Mike,

Thanks -- I'll take a closer look at your paper on this! I think we all basically agree that linear analysis of EXAFS can work, but also that compared to linear analysis of XANES, linear analysis of EXAFS has a few more caveats and issues that need to be addressed for each case.

On Mon, Aug 13, 2018 at 8:26 PM Martin McBriarty wrote:

...

Matt,

Glad to read your impressions of EXAFS LCF. I've had reasonable success with LCF using EXAFS spectra generated by ab initio molecular dynamics (AIMD) to figure out the local structure of dopants whose preferred coordination is symmetrically dissimilar from the crystals they inhabit, i.e. for which there are no good experimental standards. This can be pretty tough to do accurately with shell-by-shell fitting.

As you point out, disorder is a huge hurdle (in both LCF and shell-by-shell EXAFS analysis). We assume that a good AIMD model will simulate thermal disorder pretty well, but there are likely differences in configurational disorder between a periodic infinite structure and the real material due to defects. Fortunately, defects can be explicitly accounted for in a simulation, assuming you have the computational capability to screen a set of defect configurations.

Background subtraction should ideally be done using the same procedure for all data. Theoretical data could be used to refine a background subtraction procedure; spline fit parameters such as Rbkg or clamping may be tweaked to improve agreement between a simulated chi(k) and a measured standard over a reasonable k-range.

Simulating spectra with a range of binding energy offsets can explicitly address the problem of E0 choice, but it can also be used as a fudge factor for strain. In my LCFs, dE0 is the only parameter besides the fractions of the chosen phases.

To address the above problems, benchmarking is key. Quantitative agreement should be sought between simulated spectra and experimental standards to ensure the theory is sound and the chi(k) extraction is reasonable. However, there are probably still systematic sources of error which are larger than the uncertainties Athena's LCF tool will report; I agree with Mike's practical estimate of 10% or so.

I discuss these issues in somewhat greater detail in my recent (open access!) article that demonstrates how LCF using AIMD-simulated spectra yields answers that shell-by-shell fitting struggles with due to multiple overlapping components: https://pubs.acs.org/doi/10.1021/acs.est.8b00297

Martin

On Sun, Aug 12, 2018 at 10:19 PM, Matt Newville < newville@cars.uchicago.edu> wrote:

...

Hi Mike,

On Thu, Aug 9, 2018 at 10:04 PM Mike Massey wrote:

...

This is interesting. Could you say more about your skepticism of the robustness of EXAFS LCF, Matt?

To be fair, it suffers from many of the same drawbacks of XANES LCF, plus others. But I'm curious about your thoughts on it since yours seems to be what amounts to a "strong opinion" on the subject.

I would not say that no one should ever do linear combination fitting for EXAFS. For sure, linear analysis of XANES is quite robust and verified many times to give good results, at least at level of a few percent. Linear analysis of EXAFS suffers more data processing challenges and conceptual problems that limit its robustness. For sure, there are cases for which it can work well.

Longer answer: Any linear analysis (LCF, PCA, MCR-ALS, etc) of XANES works reasonably well (typically to a few percent) because: a) the processing needed is minimal. Data need to have a common energy calibration better than the intrinsic energy resolution -- typically energy calibration of 0.25 eV or better will be OK. Data need to have a consistent normalization of mu(E), typically to a few percent. Variations in these processing steps will have a direct and negative effect on the results.

b) conceptually, the assumption is that there exists a nearly 1 to 1 correspondence between "local chemical configuration" and "measured XANES", and that the "local chemical configurations" that are being investigated are discrete and well-defined (ie "iron carbonate") and not continuous. That is, if you determine that your Fe XANES spectra is "50% iron carbonate and 50% iron sulfate" then implicit conclusion is that 50% of the iron atoms are iron carbonate and 50 percent are iron sulfate, not that all irons are 50% carbonate and 50% sulfate.

To be clear, linear analysis of XANES does not work well to ppm levels, partly due to the poor experimental contrast (that is, mu(E) tend to all look alike and features are intrinsically broadened to the ~eV level), but also conceptually, because at the ppm level, local chemical configurations are not always limited to 3 to 10 discrete states.

Linear Combination EXAFS is more challenging from both the processing and conceptual point of view.

For Processing, EXAFS requires more data processing than XANES. The selection of E0 and the background mu0(E) will have an effect on linear analysis of EXAFS if not done consistently. It is not really obvious how E0 or mu0(E) can be selected consistently for very different spectra.

Conceptually, EXAFS is much more sensitive to disorder and subtle variations in the bond lengths (thermal or static disorder) and can have significant variation in its sensitivity to second and further neighbors. In that sense, EXAFS is much less discrete and much more continuous in its variability across different kinds of local structures.

Again, this is not to say that linear analysis of EXAFS cannot ever work, just that is probably more limited in applicability and absolute accuracy than linear analysis of XANES. Of course, for EXAFS you can also do an actual fit of structural parameters. The information content is somewhat limited so that refining multiple overlapping components may not always be possible, and linear combinations of end-member spectra may look attractive....

Hopefully, anyone who has other insights or experiences will be able to correct any of my misunderstandings.

--Matt

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