Dear All,

thank you for the comments and suggestions. It was a silly mistake on our end + rigid instructions in the tutorial I made:

1) The structure referred to as "no RMT reduction" was not 0% reduction at all (as Peter guessed). It was initialized with
        init_lapw -b -vxc 13 -rkmax 7 -numk 300
instead of the tutorial recommendation
        init_lapw -b -vxc 13 -red 3 -rkmax 7 -numk 300
leading to R(Ta)=R(As)=2 bohr. There is in fact a lot of interstitial space between MT radii and still no core leakage.

2) Because of significantly smaller RMTs compared to the tutorial, the Kmax also changed significantly causing a large change in the Fermi energy. The resultant Fermi energy becomes 0.917 Ry vs 0.801 Ry in the tutorial. Since the band structure is plotted within a narrow energy window +/- 1 eV, we saw the adjacent low-energy part of the same band structure.

Thank you all for the help once again!

Best regards
Oleg

--
Oleg Rubel (PhD, PEng)
Department of Materials Science and Engineering
McMaster University
JHE 359, 1280 Main Street West, Hamilton, Ontario L8S 4L8, Canada
Email: rub...@mcmaster.ca
Tel: +1-905-525-9140, ext. 24094
Web: http://olegrubel.mcmaster.ca

On 2019-11-05 14:00, Peter Blaha wrote:
Dear Oleg,

I cannot reproduce this.

Using RMTs of 2.5 /2.38 (this is what setrmt gives without any reduction) I get basically the same band structure as yours with reduction.

Maybe you did not execute setrmt at all and have RMT=2.0 ??  Then the SO effect would only be taken partly into account.



Am 05.11.2019 um 18:40 schrieb Oleg Rubel:
Thank you for the comments!

There is no leakage with any reduction used. The init_lapw runs clean (no warnings). There are very tiny changes in RMTs when going from 0.5% to 0% reduction.

Best regards
Oleg


On 11/5/2019 11:43 AM, Laurence Marks wrote:
Remember, SOC is only within the RMTs, see http://www.wien2k.at/events/ws2017/notes/Rocquefelte-Relativity-NCM.pdf

N.B., if the RMTs are too large you may also have leakage. For instance, with NiO (for instance) if too large an RMT is used for the Ni the O 2p states can leak into the Ni RMT which can lead to anomalies with +U or -eece.

On Tue, Nov 5, 2019 at 10:28 AM Oleg Rubel <rub...@mcmaster.ca <mailto:rub...@mcmaster.ca>> wrote:

    Dear Wien2k Community,

    I compute the band structure of TaAs. The steps are set in the tutorial     file "TaAs topological.pdf" available via the download link below. In
    the tutorial, I recommended a 3% RMT reduction even though the
    structural relaxation is not intended. With this settings, it is
    possible to get the band structure (see file "with-SOC.pdf"), which is
    very similar to the literature.

    However, if the RMT redirection is skipped during initialization (RMT     redirection = 0), the band structure transforms drastically (see file     "with-SOC.pdf"). It seems that the value of the gap between spheres is
    not important. It is important to have it (even 0.5% is OK).
    Interestingly, the presence of a gap between MT spheres affects the
    band
    structure only when SOC is present. The band structure is _not_
    sensitive to the presence of a gap between MT spheres without SOC (see
    file "without-SOC.pdf").

    As far as I understand, the wave function is continuous in the value
    and
    slope at the interface between MT region and the interstitial (plane
    wave) region. Perhaps, this condition is not fulfilled in the point
    where two MT spheres touch each other? What I do not understand is why
    it has such profound consequences only with SOC? Any thought will be
    appreciated.

    Thank you in advance.

    Best regards
    Oleg

    Files download link (avalable for 7 days):
https://urldefense.proofpoint.com/v2/url?u=https-3A__wetransfer.com_downloads_eabd33ab1535992fd1a610b8423aaf9420191105154634_71ff8dc7d5840ed6b1c9703135c1cb8420191105154634_44d984&d=DwICAg&c=yHlS04HhBraes5BQ9ueu5zKhE7rtNXt_d012z2PA6ws&r=U_T4PL6jwANfAy4rnxTj8IUxm818jnvqKFdqWLwmqg0&m=VggiwdRvos4hS2m6aY8z55ptzMRHvrcvRtpXkOVPX1I&s=z2PxBovEK4VE4a2Q1GsDsNZ2Xi2g5f33dhdv63f6TyY&e=


    --     Oleg Rubel (PhD, PEng)
    Department of Materials Science and Engineering
    McMaster University
    JHE 359, 1280 Main Street West, Hamilton, Ontario L8S 4L8, Canada
    Email: rub...@mcmaster.ca <mailto:rub...@mcmaster.ca>
    Tel: +1-905-525-9140, ext. 24094
    Web:
https://urldefense.proofpoint.com/v2/url?u=http-3A__olegrubel.mcmaster.ca&d=DwICAg&c=yHlS04HhBraes5BQ9ueu5zKhE7rtNXt_d012z2PA6ws&r=U_T4PL6jwANfAy4rnxTj8IUxm818jnvqKFdqWLwmqg0&m=VggiwdRvos4hS2m6aY8z55ptzMRHvrcvRtpXkOVPX1I&s=CAxx1qmO-zULEZwepo5VowgIZSez-bLvWebZmAuX4Gs&e=

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--
Professor Laurence Marks
Department of Materials Science and Engineering
Northwestern University
www.numis.northwestern.edu <http://www.numis.northwestern.edu/>
Corrosion in 4D: www.numis.northwestern.edu/MURI <http://www.numis.northwestern.edu/MURI>
Co-Editor, Acta Cryst A
"Research is to see what everybody else has seen, and to think what nobody else has thought"
Albert Szent-Gyorgi

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