Re: [Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-21 Thread Peter Blaha

Emax seems converged. This is no issue.

Yes, from my point of view the "best" calculation should be to put 5p in 
core (+ .locre if necessary) and have the 6p RLO. It seems it has a 
rather large effect.


To check my results I would:

a) Calculate the qtl's with p-1/2 p3/2 splitting (x qtl -so) and check 
that within these bands there is significant character of p1/2 or p3/2. 
(Character-plot with band structure), which varies from Gamma-X 
explaining the importance of the p1/2 RLO.


b) Do a calculation without symmetry (P1) and calculate the bands in 
different "equivalent" directions of the BZ. I'd like to see that there 
is no symmetry-bug related to the RLOs.


c) I'd also would reconfirm, that after an scf calculation with SO but 
WITHOUT RLO, and just doing the bandstructure with and without RLO 
(non-selfconsistent) one gets more or less the same change (or is it an 
scf-effect ?). In addition, is the sum of eigenvalues (case.scf2) after 
lapw2 lower with RLO (check of variational principle).


In any case, looks interesting 

What says experiment ???

Am 21.12.2016 um 21:50 schrieb Martin Gmitra:

Thanks for replay!

Considering the RLO for 6P (0.3 Ry), it strengthen the spin-orbit
coupling effects rather significantly, comparable to results when
considering RLO for 5P at -8Ry, see yellow and dark red curves in the
attached plot.

Can one understand this as the orthogonality effect as you have suggested?

Important observation is that dispersions with RLO for 5P in valence
and RLO for 6P (with 5P in core) is different (yellow and dark red
curves). Anyhow, I am getting impression from your argumentation that
the correct practice would be to take 5P for core + .lcore and add the
RLO for the 6P unoccupied states, right?

If one considers this case (results shown by dark red curve, RLO for
6P) as an benchmark, results obtained when enlarging Emax up to 45 Ry
(blue plus symbols) can be assumed as converged (compare orange, green
and blue curves) but hardly reach the case with RLO for 6P. There is
still a difference of about 0.1 eV.

What do you think about the observed differences?

Do you think is there a sense to increase the Emax even more? (How to
get even more bands without increasing Rkmax?)

Best regards,
Martin Gmitra
Uni Regensburg



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Re: [Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-21 Thread Martin Gmitra
Thanks for replay!

Considering the RLO for 6P (0.3 Ry), it strengthen the spin-orbit
coupling effects rather significantly, comparable to results when
considering RLO for 5P at -8Ry, see yellow and dark red curves in the
attached plot.

Can one understand this as the orthogonality effect as you have suggested?

Important observation is that dispersions with RLO for 5P in valence
and RLO for 6P (with 5P in core) is different (yellow and dark red
curves). Anyhow, I am getting impression from your argumentation that
the correct practice would be to take 5P for core + .lcore and add the
RLO for the 6P unoccupied states, right?

If one considers this case (results shown by dark red curve, RLO for
6P) as an benchmark, results obtained when enlarging Emax up to 45 Ry
(blue plus symbols) can be assumed as converged (compare orange, green
and blue curves) but hardly reach the case with RLO for 6P. There is
still a difference of about 0.1 eV.

What do you think about the observed differences?

Do you think is there a sense to increase the Emax even more? (How to
get even more bands without increasing Rkmax?)

Best regards,
Martin Gmitra
Uni Regensburg
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Re: [Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-15 Thread Peter Blaha

Is this all converged with respect to EMAX in case.in1 ???

So from your figure one would find that these bands at EF are affected 
by >0.1 eV when you add a p1/2 basis function at -8 Ry 


This sounds VERY strange to me and I don't know if one can explain this 
by an "orthogonality effect" (If the 5p-1/2 state is better described 
due to this basis, the 6p-1/2 must be orthogonal to them and thus are 
also affected).


What I would do is to check what comes out by putting the 5p in core, 
but then try to add a RLO with an energy=0.3 (a 6p-RLO).



Charge leakage does not seem to have an effect as seen in your plot or 
according to your statement that you get the same reults with a 
different RMT.



On 12/15/2016 10:59 AM, Martin Gmitra wrote:

Dear Peter,

Thank you for your answer.

The main reason to use the RLO is the effect close to the Fermi level,
where the top valence and bottom conduction bands are strongly pushed
towards each other due to spin-orbit coupling.

In the attached figure you can find plot for the different cases. The
blue line is for the 5P in valence without RLO, adding RLO, red line,
the band inversion is strongly enhanced.

When 5P are in core, the effect of band inversion is sort of in
between the cases without RLO and with RLO, see green and violet
dashed curves. Effect of .lcore is rather minor, compare the green and
violet lines. The spheres we consider are 2.5 a.u., and 5P in the core
gives charge leakage of 0.003020. For the larger spheres of 2.7 a.u.,
the core charge leakage reduces to 0.001118, but resulting band
structure (using .lcore as well) is pretty the same as the violet one,
not shown in the figure.

Could you comment please what is the good criteria to decide whether
the leakage is small or not?

I would be very glad you could comment on the RLO effect to the band
inversion and give your statement which calculations are more correct?

Best regards,
Martin Gmitra
Uni Regensburg



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Re: [Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-15 Thread Martin Gmitra
Dear Peter,

Thank you for your answer.

The main reason to use the RLO is the effect close to the Fermi level,
where the top valence and bottom conduction bands are strongly pushed
towards each other due to spin-orbit coupling.

In the attached figure you can find plot for the different cases. The
blue line is for the 5P in valence without RLO, adding RLO, red line,
the band inversion is strongly enhanced.

When 5P are in core, the effect of band inversion is sort of in
between the cases without RLO and with RLO, see green and violet
dashed curves. Effect of .lcore is rather minor, compare the green and
violet lines. The spheres we consider are 2.5 a.u., and 5P in the core
gives charge leakage of 0.003020. For the larger spheres of 2.7 a.u.,
the core charge leakage reduces to 0.001118, but resulting band
structure (using .lcore as well) is pretty the same as the violet one,
not shown in the figure.

Could you comment please what is the good criteria to decide whether
the leakage is small or not?

I would be very glad you could comment on the RLO effect to the band
inversion and give your statement which calculations are more correct?

Best regards,
Martin Gmitra
Uni Regensburg
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Re: [Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-14 Thread Peter Blaha
This is related to the fact, that the RLOs are implemented without 
symmetry constrains (and relativistic spherical harmonics basis) and for 
numerical reasons this leads to these small splittings. This is also 
noted when calculating EFGs, that one must not use RLOs.


Why are you using RLOs and the Bi 5p states as valence anyway ? States 
at -8 Ry should usually be kept in the core, unless one has very good 
reasons not to do so (high pressure calculations). Treating them as 
core, they get the full relativistic treatment (have proper j-based 
radial wave functions) and this description is much better than a 
"band-treatment" with a scalar-relativistic basis (l-based), where the 
band-width is usually much smaller that spin-orbit effects.


The Bi spheres should be sufficiently large and eventual small core 
leakage can be treated using the automatic way with .lcore.



The change in energy between lstart and lapw1 is due to a shift in 
potential. In lstart we have an energy-zero = 0 at infinity, in lapw we 
have another energy zero.


On 12/14/2016 07:58 AM, Martin Gmitra wrote:

Dear Wien2k users,

I am facing a problem with symmetry preserved result when relativistic
local orbital (RLO) is added to the spin-orbit coupling calculations.

The system is bismuthene, a 2D layer of Bi atoms, in orthorombic
lattice WITH inversion.

Without RLO the bands are doubly degenerated, up to numerical
precision below 1 micro eV, (correct result).

By adding RLO for 5P_1/2 (found by autosearch to -8.08 Ry, close to
the -8.3 Ry from lstart) the bands split. For the top valence band it
can reach values of several meV (!), see plot in the attachment.
It stays degenerate at Gamma point while at the other time-reversal
invariant points (X, Y, and S point in the plot) it does not.

My question is:
How to improve precision?
Do you have any idea what could be reason for and provide possible
hint how to solve the problem?

Another (perhaps minor) point:
Autosearch finds RLO at -8.08 Ry while lstart finds for 5P_1/2 value
-8.3 Ry, what is behind the 0.2 Ry renormalization?

Note 1:
Calculations done by version 14.2, XC_PBESOL and default basis type
used, increasing Emax and Rmax do not improve results, the "ghost"
splitting stays there.

Note 2:
Wien2k version 16 gives similar results.
For intallation -- I had to patch the siteconfig script commenting line 148
if("$test" != "/") goto iloop
otherwise it runs into the infinite iloop if the FFTWl_LIBS are not set up.


Best regards,
Martin Gmitra
Uni Regensburg



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Phone: +43-1-58801-165300 FAX: +43-1-58801-165982
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[Wien] incorrect band splitting when RLO added for a system with spatial inversion

2016-12-13 Thread Martin Gmitra
Dear Wien2k users,

I am facing a problem with symmetry preserved result when relativistic
local orbital (RLO) is added to the spin-orbit coupling calculations.

The system is bismuthene, a 2D layer of Bi atoms, in orthorombic
lattice WITH inversion.

Without RLO the bands are doubly degenerated, up to numerical
precision below 1 micro eV, (correct result).

By adding RLO for 5P_1/2 (found by autosearch to -8.08 Ry, close to
the -8.3 Ry from lstart) the bands split. For the top valence band it
can reach values of several meV (!), see plot in the attachment.
It stays degenerate at Gamma point while at the other time-reversal
invariant points (X, Y, and S point in the plot) it does not.

My question is:
How to improve precision?
Do you have any idea what could be reason for and provide possible
hint how to solve the problem?

Another (perhaps minor) point:
Autosearch finds RLO at -8.08 Ry while lstart finds for 5P_1/2 value
-8.3 Ry, what is behind the 0.2 Ry renormalization?

Note 1:
Calculations done by version 14.2, XC_PBESOL and default basis type
used, increasing Emax and Rmax do not improve results, the "ghost"
splitting stays there.

Note 2:
Wien2k version 16 gives similar results.
For intallation -- I had to patch the siteconfig script commenting line 148
if("$test" != "/") goto iloop
otherwise it runs into the infinite iloop if the FFTWl_LIBS are not set up.


Best regards,
Martin Gmitra
Uni Regensburg
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