The ghostbands are for Sn-d states.

The case.in1 file shows 2 lines for the d-states, a shallow LO for semicore + APW for valence.

I asked you, what the actual energies in case.scf1 are. Without this, I can only speculate that the E-LO and E-APW are too close together for Sn-d.

My suggestion is to increase the E-parameter for all Sn-d from 0.3 to eg. 1.3 and rerun the scf cycle. When this works, restore the original 0.3 value after a couple of iterations.

Am 04.02.2020 um 20:28 schrieb Laurence Marks:
If it is in the first cycle, this is a nasty problem that arises because the initial density is not always very good. I think you are going to have to adjust (by hand) the RMTs until you find something which avoids this problem. Later you can use expand_rmt_lapw (which works for changes as well) to adjust. My hunch is to use a larger RMT for Sn, e.g.

setrmt case -a Na:2.0,Fe:1.9,Sn:2.0,O:1.7
cp case.struct_setrmt case.struct

(replace "case" by whatever"). Then run "x lstart ; x dstart ; x dstart -up ; x dstart -dn" and try again. So long as you can get past the first interaction you will be up and running.

N.B., Peter may have some other ideas.

On Tue, Feb 4, 2020 at 12:30 PM Biswajit Mandal <[email protected] <mailto:[email protected]>> wrote:

    Dear sir,
    Thank you very much for your suggestions.
    I have again simulated with -7.0Ry separation energy and encountered
    the same error in first cycle. For this calculation, the parent
    material is NaFeSnO4 which is an anti-ferromagnetic material
    confirmed experimentally. The anti-ferromagnetic nature arises due
    to antiparallel spin orientation of Fe atoms, distributed in two
    different 4c sites. Each of these 4c sites are equally shared by Fe
    and Sn atom. In this case, we have broken symmetry using vasp and
    run spin-polarized calculation with GGA+U scheme. For Fe atoms we
    have taken Ueff=6eV. The case.inst for this simulation is as follows;
    Na
    Ne 1
    3,-1,0.5  N
    3,-1,0.5  N
    Na
    Ne 1
    3,-1,0.5  N
    3,-1,0.5  N
    Fe
    Ar 3
    3, 2,2.0  N
    3, 2,2.0  N
    3,-3,0.0  N
    3,-3,2.5  N
    4,-1,0.5  N
    4,-1,1.0  N
    Fe
    Ar 3
    3, 2,2.0  N
    3, 2,2.0  N
    3,-3,2.5  N
    3,-3,0.0  N
    4,-1,1.0  N
    4,-1,0.5  N
    Sn
    Kr 5
    4, 2,2.0  N
    4, 2,2.0  N
    4,-3,3.0  N
    4,-3,3.0  N
    5,-1,1.0  N
    5,-1,1.0  N
    5, 1,1.0  N
    5, 1,1.0  N
    5,-2,0.0  N
    5,-2,0.0  N
    Sn
    Kr 5
    4, 2,2.0  N
    4, 2,2.0  N
    4,-3,3.0  N
    4,-3,3.0  N
    5,-1,1.0  N
    5,-1,1.0  N
    5, 1,1.0  N
    5, 1,1.0  N
    5,-2,0.0  N
    5,-2,0.0  N
    Fe
    Ar 3
    3, 2,2.0  N
    3, 2,2.0  N
    3,-3,2.5  N
    3,-3,0.0  N
    4,-1,1.0  N
    4,-1,0.5  N
    Fe
    Ar 3
    3, 2,2.0  N
    3, 2,2.0  N
    3,-3,0.0  N
    3,-3,2.5  N
    4,-1,0.5  N
    4,-1,1.0  N
    Sn
    Kr 5
    4, 2,2.0  N
    4, 2,2.0  N
    4,-3,3.0  N
    4,-3,3.0  N
    5,-1,1.0  N
    5,-1,1.0  N
    5, 1,1.0  N
    5, 1,1.0  N
    5,-2,0.0  N
    5,-2,0.0  N
    Sn
    Kr 5
    4, 2,2.0  N
    4, 2,2.0  N
    4,-3,3.0  N
    4,-3,3.0  N
    5,-1,1.0  N
    5,-1,1.0  N
    5, 1,1.0  N
    5, 1,1.0  N
    5,-2,0.0  N
    5,-2,0.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    O
    He 3
    2,-1,1.0  N
    2,-1,1.0  N
    2, 1,1.0  N
    2, 1,1.0  N
    2,-2,1.0  N
    2,-2,1.0  N
    ****
    ****         END of input (instgen_lapw)
    Is this approach wrong? If wrong, then kindly help me to break the
    symmetry so that I could get some meaningful result.
    Thanks in advance
    With regards

    On Tue, Feb 4, 2020 at 9:33 PM Laurence Marks
    <[email protected] <mailto:[email protected]>> wrote:

        Several other points:
        1) It appears that you did not to follow the standard
        initiation. Your atom positions have errors, for instance atom 2 is
        ATOM  -2: X=0.77850183 Y=0.75000002 Z=0.15072562  and should be
        ATOM  -2: X=0.77850183 Y=0.75000000 Z=0.15072562
        This can matter. With this corrected Wien will (properly) switch
        axes to put the mirror down z.

        2) It looks like you used a non-standard energy in lstart, to
        avoid core leaking. These are warnings, and you should not
        adjust too much particularly when you have a complex structure
        with (perhaps) inaccurate atomic positions. I suggest just using
        -7, your use of -10 (?) was not needed.

        3) Beware that Vasp can reduce symmetry inappropriately. I would
        start of with the published Pnma symmetry and occupy one of the
        Fe sites and one of the Sn sites.

        4) You will need to look into the magnetism. I don't know if
        this is ferromagnetic or anti-ferromagnetic. If the later you
        will need to break the symmetry appropriately (carefully).

        5) I doubt that you will get meaningful results unless you use
        either -eece or +U for the Fe sites.

        On Tue, Feb 4, 2020 at 9:25 AM Peter Blaha
        <[email protected]
        <mailto:[email protected]>> wrote:

            Does the problem happen in the first scf cycle or later on ???

            If it is later, make sure :NEC01 is ok in the scf fle.

            Check case.scf1 to see where the actual E-parameters for
            atom 5 l=2 are.
            If the E-parameters for APW and for the LO are too close
            ---> ghostbands


            Are you sure you need the Sn-s semicore states ??



-- 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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-- Yours Sincerely
    ------------------------
    Biswajit Mandal
    PhD Research Scholar
    Department of Physics
    IIT Patna
    Bihta, Patna-801103
    INDIA
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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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