Matt and Max,

Thank you for your responses, the information was really helpful in trying to 
understand what would lead to the changes in Io between scans.  My knowledge of 
the infrastructure and mechanics of the beamline in front of Io is limited, and 
this short discussion has been very insightful. I wanted to make clear I was 
not trying to call out a specific issue with a beamline, but rather better 
inform myself about the how beamlines in general are setup and the mechanics 
behind it.

It is hard to find a specific text or manuscript that covers topics along this 
line.  Not just with XAFS, the same could be said about a number of other 
spectroscopy/analytical techniques.  Being able to pose questions of this 
nature to the list is really helpful and provides an insight and source of 
information that is not readily available.

All the Best,

Todd Luxton, Ph.D.
Office of Research and Development
National Risk Management Research Laboratory
Land Remediation and Pollution Control Division
Waste Management Branch

Mailing Address:
5995 Center Hill Ave
Cincinnati, OH 45243

Phone:
Office: (513) 569-7210
Cell: (513) 319-5104
Fax: (513) 569-7879

Email: luxton.t...@epa.gov<mailto:luxton.t...@epa.gov>

“A nation that destroys its soils destroys itself”
Franklin D. Rosevelt

From: Ifeffit [mailto:ifeffit-boun...@millenia.cars.aps.anl.gov] On Behalf Of 
Matt Newville
Sent: Thursday, March 31, 2016 6:41 PM
To: XAFS Analysis using Ifeffit <ifeffit@millenia.cars.aps.anl.gov>
Subject: Re: [Ifeffit] Question about Io during data collection

Hi Todd,


On Thu, Mar 31, 2016 at 9:27 AM, Luxton, Todd 
<luxton.t...@epa.gov<mailto:luxton.t...@epa.gov>> wrote:
All:

Recently our group was at the APS collecting Pb L(III) spectra on an ID line 
using quick XAFS.  Data was collected from -200 to +800 eV for Pb L(III) at 0.2 
eV steps with a count rate of 0.025 seconds.  Each scan took about 2.5 minutes 
to complete.   During our measurements we began noting issues with the 
linearity of scans collected in the extended region of the same sample.  After 
poking around in the data we noticed that Io was not linear throughout the 
measurement for a portion of the scans.  This was not always the true (see 
Athena project attached to the email, and images attache to the email).  I was 
always under the impression that Io should ideally remain linear throughout the 
energy region scanned, or at least remain unchanged between replicate scans.  
We worked with the beamline scientists to try alleviate/fix the issue, but it 
kept persisting.   I realize this is not an IFEFFIT issue, but I was hoping 
someone might be able to help me understand what was going on and why this was 
happening?  If I have not included enough information for the question please 
let me know.

It's a little hard to see much detail from the blurry images, but I0 is 
definitely falling in dramatically different ways for the different scans.
My guess (from similar experience trying to do continuous XAFS scans at another 
APS ID line) is that the undulator is not tracking with the monochromator 
correctly in some of the scans. This tracking is definitely challenging for us. 
I suspect MR-CAT does small, constant energy steps per time point, but I'm not 
sure of this.  There is no way I can scan my undulator at 25 ms per energy 
point.
What I see (and from talking to the undulator control folks at the APS), there 
is about a 0.5 second "settling time" for the devices during which time is 
pointless to ask for another move.
So, when I do QXAFS at 13-ID-E, I set up "a normal XAFS scan", with 0.05 Ang^-1 
steps and move the mono energy between these points in a fixed time -- so doing 
a ~4 eV move per time point at 10 Ang^-1.   But I find that if I try to go 
faster than about 100 ms per point, I see oscillations in I0, as the undulator  
lags behind and then tries to catch up.   That can put oscillations in I0, but 
what you're seeing is it just falling off, like the tracking just isn't working.
For those not at the APS, the undulators cannot be hardware-synchronized 
(perhaps that is "yet", but we've been waiting a long time).  One can move the 
undulator at a constant rate in gap (mm) velocity, and then try to synchronize 
the mono energy to that... I don't do that and I'm pretty sure that MR-CAT does 
not either.

Anyway, I would suspect the tracking of the undulator.
Hope that helps,

--Matt
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