Hi Matthew, Jana,
I think the Chantler values, especially in Hephaestus, are not particularly
robust at the Ca L edges.
To be clear, Elam gives L3, L2, and L1 energies as 346.2, 349.7, and 438.4
eV, and the edge jumps as 5.8, 1.4, and 1.1. I believe those edge jumps
may have originated from Shaltout -- maybe Bruce can clarify that.
The Chantler data from the NIST FFast web page (and in Hephaestus) are
quite sparse. This is a definitely a problem for using the anomalous
scattering factors near edges. I've talked with Chris Chantler about this a
few times over the years. Not too long ago, he sent me data on a finer
grid -- but he also told be recently that he hoped to have even better data
he could send to me soon (all time-scales here on months-to-years here).
I've included the finer data I have from Chantler into Larch. But the
results for the Ca L edges are still not encouraging. The attached figure
and ASCII data file give the results for mu(E) (gr/cm^2) from Elam and from
Chantler. It's hard to see an L2 edge in either, and Chantler does not
show an L1 edge.
FWIW, the script to generate this is:
####################
energies = linspace(300, 500, 101)
muca_chantler = mu_chantler('Ca', energies)
muca_elam = mu_elam('Ca', energies)
newplot(energies, muca_chantler, ymax = 50000, label='Chantler')
plot(energies, muca_elam, label='Elam')
info_head = 'Ca edge Energy(eV) Fyield EdgeJump'
info_l3 = ' L3 %.1f %.5f %.2f' % xray_edge('Ca', 'L3')
info_l2 = ' L2 %.1f %.5f %.2f' % xray_edge('Ca', 'L2')
info_l1 = ' L1 %.1f %.5f %.2f' % xray_edge('Ca', 'L1')
write_ascii('CaMu.dat', energies, muca_elam, muca_chantler,
info_head, info_l3, info_l2, info_l1,
label='Energy MuCa_Elam MuCa_Chantler')
########################
I'm not sure that gives a lot of insight except that not trusting
Chantler's values for these values might be reasonable.
On Thu, Sep 24, 2015 at 10:16 AM, Matthew Marcus
I'm not after absolute data, just the edge-jump ratio. This would have to be extracted by peak+arctan fitting because any spectra will have peaks and a very limited range between edges. If the Chantler numbers are incorrect, then perhaps the edge-jump ratio is really 2.
Do you have a reference which can be cited?
I'll try the CXRO tool next, since CXRO specializes in soft X-rays. mam
On 9/23/2015 11:49 PM, Jana Padeznik Gomilsek wrote:
It is very hard to measure or to calculate absolute absorption data, especially in the vicinity of the absorption edges and especially in the soft x-ray region. Therefore there are significant differences between the tables and I think nobody knows which are better. Chantler, for example, says the expected uncertainties of the tables in your region are 50 % to 100 % ( http://physics.nist.gov/PhysRefData/FFast/Text2000/sec06.html#tab2). I would doubt the Chantler's L3+.1 number, all other numbers look ok - this is what you can get.
jana padeznik gomilsek
Message: 3
Date: Wed, 23 Sep 2015 18:02:08 -0700 From: Matthew Marcus
To: XAFS Analysis using Ifeffit Subject: [Ifeffit] Problem with Hephaestus at Ca L-edges Message-ID:<56034B90.70405@lbl.gov> Content-Type: text/plain; charset=utf-8; format=flowed I wanted to work out the edge-jump ratio between the L3 and L2 edges of Ca using Hephaestus. I ran into two problems:
1. The ratio implied by what it says for the unit-edge-step thickness does not agree with that derived by computing the absorption (cm^2/gm) above and below each edge and dividing the difference (L3+ - L3-)/(L2+ - L2-).
2. The results differ wildly depending on which resource I use:
L3-.1 L3+.1 L2-.1 L2+.1 (L1+ - L1-)/(L2+ - L2-) Elam 4759.796 27837.796 27478.018 38434.277 2.106375908 Chantler 4322.6 6547.121 32827.61 35436.543 0.852655473 Cromer-Leiberman 4288.524 33471.375 32786.294 47072.991 2.042659055
The Henke table doesn't yield an L2 edge jump at all, while the Shaltout yields the same results as Cromer-Leiberman. Which one should I trust and why?
This is old-style H. (V0.18), not Demeter. mam
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--Matt