[Wien] Q: charge lost in SO calculation depending on LAPW / APW+lo
Torsten Andersen
thor at physik.uni-kl.de
Wed Nov 16 08:14:23 CET 2005
Dear Dr. Zijlstra,
one suggestion on its cause:
The spin-orbit interaction (s.o.c.) is only implemented inside the
muffin-tins. You can test the influence of this by maximizing the size
of the muffin-tins and see if the loss gets smaller.
Also, it (s.o.c.) is implemented in second variation, so you need to
include the spin-orbit in the whole SCF cycle in order to get reliable
results. I am not sure that second variation is bulletproof, but usually
it works.
Best regards,
Torsten Andersen.
Eeuwe Sieds Zijlstra wrote:
> Dear all,
>
> For bismuth (Bi) I found the following behavior, which I do not understand:
>
> When 6s states were described by LAPW's and 6p states by APW+lo's
> and when the spin-orbit (SO) interaction was included using a relativistic
> local p1/2 orbital, 0.33 electrons were lost as can be seen from the
> following output of MIXER:
>
> :NEC01: NUCLEAR AND ELECTRONIC CHARGE 83.00000 82.67338 1.00395
>
> This charge disappears from the p channel as can be seen when QTL is compared
> for the above case and a case where the 6s states are also described by
> APW+lo's:
>
> :QTL001: 1.2922 1.3993 9.8302 0.0642 .... (above case)
> :QTL001: 1.2631 1.7246 9.8203 0.0643 .... (when 6s is described by APW+lo's)
>
> No charge was lost when 6s was described by APW+lo's, when 6s and 6p were both
> described by LAPW 's (but this calculation is unstable, so I did just one
> iteration), or when no p1/2 orbital was included.
>
> I checked that there are no linear dependencies in the second-variational
> secular equation (the overlap matrix is positive definite) and that this
> behavior does not depend on Emax or the choice of basis for the d states,
> i.e., APW+lo or LAPW. There were no QTL-B warnings or other warnings that I
> am aware of.
>
> When no p1/2 orbital orbital was included, the total energy was insensitive to
> whether LAPW or APW+lo was used for 6s and 6p, so in principle these choices
> form an equally good basis for LAPW1
>
> I found this behavior for both the A7 structure (with 2 atoms per unit cell)
> and for simple cubic Bi [space group Pm-3m (number 221), a = 6.18 Bohr,
> Gamma point only with temperature smearing, Eval=0.001 Ry]. The above data are
> for the latter calculation, which is simpler. For this calculation my files
> case.in1 and case.inso are:
>
> ********* case.in1 *************
> WFFIL (WFPRI, SUPWF)
> 7.00 10 4 (R-MT*K-MAX; MAX L IN WF, V-NMT
> .07680 4 0 global e-param with N other choices, napw
> 0 -0.364 0.010 CONT 0
> 1 0.205 0.000 CONT 1
> 2 -1.273 0.010 CONT 0
> 2 0.113 0.000 CONT 0
> K-VECTORS FROM UNIT:4 -4.0 0.9 emin/emax window
> ********** end of case.in1 ************
>
> ********* case.inso ***********
> WFFIL
> 4 4 0 llmax,ipr,kpot
> -10.0000 0.90000 emin,emax (output energy window)
> 0. 0. 1. direction of magnetization (lattice vectors)
> 1 number of atoms for which RLO is added
> 1 0.205 0.000 CONT
> 0 0 0 0 0 number of atoms for which SO is switch off;atoms
> ********** end of case.inso ************
>
> Finally, I checked that this same behavior occured both with the precompiled
> WIEN2k package and when I compiled WIEN2k with the Portland Group compiler
> pgf90, with and without optimization.
>
> My question is, whether anyone has had similar problems? Whether somebody
> could comment on its cause? I would really like to know, whether there is a
> bug in the program or whether there is some criterium according to which I
> can choose my basis set in one way but not in another way and of which I am
> not aware.
>
> I hope that this question is not too hard.
> Any help would of course be greatly appreciated!
>
>
> Sincerely,
>
> Eeuwe Sieds Zijlstra
> Theoretical Physics
> University Kassel
> Germany
> _______________________________________________
> Wien mailing list
> Wien at zeus.theochem.tuwien.ac.at
> http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
>
--
Dr. Torsten Andersen TA-web: http://deep.at/myspace/
AG Hübner, Department of Physics, Kaiserslautern University
http://cmt.physik.uni-kl.de http://www.physik.uni-kl.de/
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