, it
seems that this factor has no effect on the spectral shape (although it does
modify the absolute intensity) for K-edge spectra and has a small but possibly
significant effect on L3-edge spectra (usually a relative increase in the
amplitude of the spectrum at lower energies).
Thanks,
John
that hfsd.f returned only an r-weighted Dirac spinor rather than an
r^2-weighted spinor.
I am sure you are correct though, I thought it very strange that the XSPEC code
would be missing the dipole operator in the radial part.
Thanks again,
John McLeod
On 2011-09-26, at 2:48 PM, Kevin Jorissen
a reasonably accurate band gap - so I find it a bit
curious that my approach fails for FeO.
I would greatly appreciate a quick tip on how the original calculations
in PRL 102 226401 were performed.
Regards,
John McLeod
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On Thu, 10 Dec 2015, John McLeod wrote:
Hello all,
I tried to calculate the electronic structure of FeO using mBJ.
1. I took the cubic FeO structure, made a 2x2x2 primitive
supercell, relabeled the Fe sites "1" and "2" to get the appropriate
AFM ordering, ran sgrou
situation.
Regards,
-John McLeod
So I do not think SOC can be
On 2016-11-10 10:02 PM, Peter Blaha wrote:
I'm not the expert on that topic, but I think you mix up the two
dielectric constants, which could be a semantic problem. To compare
with a classic experiment, you may need to obtain the ionic
co
To add to what Gavin said, I previously used WIEN2k to calculate
(pseudo-)cubic CH3NH3PbI3. This structure had some geometry optimization
(hence it is not a perfect cube anymore) and internal positions were
optimized with the MSR1a method.
If you want to use that structure, the atomic
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