Hi Renske,
I still think your problem is related to the potentials. If you unzip your artemis project and look in one of the feffXXXX.dat files in the folder data0.feff3 (this calculations was done with the solvent_O) you will find the calculated R_MTs in the first lines - for ipot3 (O) this is 1.6. Do the same with the data0.feff7 folder (apparently this calculation was done without the solvent O - even though the feff.inp says something different) and you will find 0.728. FEFF (always?) uses the closest atom (relative to the ipot=0-atom) to determine the unique potentials to be used for all atoms with the same ipot (in the manual it is stated that FEFF takes the first atom in the atoms-list but in your case just changing the position in the list did change nothing whereas increasing the distance to 3.3 (the O_t_1 atoms are at 3.266) did yield a different R_MT - but maybe I am wrong).
HTH
Jakob
___________________________________________________
Jakob Frommer
Soil Chemistry Group
Institute of Biogeochemistry and Pollutant Dynamics,
ETH Zürich
Universitätstrasse 16,
CHN F19
CH - 8092 Zürich
Tel: +41 44 632 87 58
Fax: +41 44 633 11 18
web: http://www.ibp.ethz.ch/research/soilchemistry
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Sent: Thu 10/2/2008 06:37
To: ifeffit@millenia.cars.aps.anl.gov
Subject: Ifeffit Digest, Vol 68, Issue 3
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Today's Topics:
1. Re: Athena Peak Fitting (Matt Newville)
2. Re: Independence of scattering paths? (van der Veen Renske)
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Message: 1
Date: Wed, 1 Oct 2008 16:23:34 -0500
From: "Matt Newville"
Hi Everyone,
I am using Athena peak fitting function to fit the sulfur spectrum of my coke sample. I checked everywhere, but couldn't get detailed instruction for using this function. So, I attached a file with this email to get help. Could you please take a look at it, and tell me if I did the fitting right (in terms of fitting procedure only)?
I did the fitting in two ways, and I know both of them have problems. For instance, in the first case, I can't get a good step line and have to cut off the tail of the spectrum. In the second one, peak 1 is way too broad, but if I cut it off, the fitting will be very poor. So, please tell me which way is better, or you have some ideas to improve the fitting.
Thank you in advance!
Best,
Jenny
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Message: 2
Date: Thu, 2 Oct 2008 06:36:48 +0200
From: "van der Veen Renske"
I have a question concerning the independence of scattering
I fitted the EXAFS signal of a molecule consisting of 30 atoms (the related FEFF calculation is called calc 1). To see the effect of the surrounding solvent molecules in the chi(k) data, I added an O-atom in the coordinate list of the FEFF input file at an arbitrary distance from the absorbing atom (in this case Pt) and I re-ran FEFF (calc 2). As a check within calc 2, I generated the sum of the same scattering paths that were used in the fitting model of calc 1 using
obtained structural fit parameters. The new O-atom was not included in this sum. I expected the sum within calc 2 to be identical to the fit of calc 1 based on the fact that the original atoms can not sense the
On Friday 26 September 2008 22:38:58 van der Veen Renske wrote: pathways. the therein presence
of the new O-atom (independence of scattering paths). BUT: the resulting sum was significantly different from the fit!
It is a little hard to answer this question since you described it to us rather than showing it to us with project file(s). I have a couple of suggestions, but without being able to examine what you did, I cannot be sure that either is relevant. (You can insert here my standard diatribe on the topic of how to ask questions.)
One suggestion is to be very careful that you are including the same set of paths in the calculation. When you add an atom to a feff.inp file, the indexing of the paths change in a way that may be hard to predict. Just blindly summing up the first N paths may not do what you want.
The other suggestion is to check that you did not place the oxygen atom in a position that dramatically altered the muffin tin radii. The potantials calculation can change quite if you insert an atom at an arbitrary loctation such that the muffin tin radii have to be very different for some atoms.
B
-- Bruce Ravel ------------------------------------ bravel@bnl.gov
National Institute of Standards and Technology Synchrotron Methods Group at NSLS --- Beamlines U7A, X24A, X23A2 Building 535A Upton NY, 11973
My homepage: http://xafs.org/BruceRavel EXAFS software: http://cars9.uchicago.edu/~ravel/software/exafs/