[Wien] optical properties calculations?
Jian-Xin Zhu
jxzhu at lanl.gov
Fri Oct 15 05:35:48 CEST 2010
Dear Peter and Respectful Wien Users,
1/
In the UG, page 147, I notice the following for the optical properties
calculations ----
In cases of non-spinpolarized calculations WITHOUT inversion symmetry
AND spin-orbit coupling,
one must do some tricks and “mimick” a spinpolarized calculation:
I cp case.vsp case.vspup Line 1
I cp case.vsp case.vspdn Line 2
I cp case.vectorso case.vectorsoup Line 3
I x lapw2 -fermi -so -c Line 4
I cp case.weight case.weightup Line 5
I cp case.weight case.weightdn Line 6
I x optic -so -up
Line 7
I x joint -up
Line 8
As I understand, the first sentence is saying that the case is non-
spin polarized but has no "Inversion symmetry" and no "spin-orbit
coupling".
Then in this case, how can the file "case.vectorso" (3rd line of the
above tricks) is created now that the spin-orbit coupling does not
exist?
However, from the lines 4 and 7, the "-so" switch is included, I
suspect the case has the "spin-orbit coupling".
On the other hand, I also read the following paragraph
In order to get the correct matrix elements, the files
case.vectorso[up|dn] have to be used.
For that purpose the following procedure is recommended:
I run SCF cycle: run[sp] lapw -so
I generate a fine k-mesh for the optics part: x kgen [-so (if
case.ksym has been
created by symmetso) ]
I change TOT to FERMI in case.in2c
I execute run[sp] lapw -so -s lapw1 -e lcore with this fine k-mesh
I run optic: x opticc -so [-up]
I run joint: x joint [-up]
I run kram: x kram [-up]
It seems the immediately above procedure should also be applicable to
the non-spin polarized case but with spin-orbit coupling.
I am confused here and very much appreciate a clarification.
2/ Another question:
Does the current "OPTICS" support the LDA+U?
Thanks,
Jianxin
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