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        <div dir="ltr" data-setdir="false">Dear Dr. Blaha</div><div dir="ltr" data-setdir="false">I act as you said, but the problem "<span><span style="font-family: Helvetica Neue, Helvetica, Arial, sans-serif; font-size: 16px;">LAPW2' - semicore band-ranges too large, ghostbands</span></span>" exists again!!</div><div dir="ltr" data-setdir="false">LO for N-2s orbitals in case.in1c were removed, but it worked just for rkm=6 (with or without LO for N).</div><div dir="ltr" data-setdir="false">I tried your way with changing rmt of atoms but the problem remained.</div><div dir="ltr" data-setdir="false"><br></div><div dir="ltr" data-setdir="false">I tried a normal scf with RKm=7, from the beginning, at a different directory, but nothing was changed. Just, crashing LAPW2 is postponed in some more cycles.</div>
        
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                    On Sunday, November 12, 2023 at 08:42:25 PM GMT+3:30, Peter Blaha <peter.blaha@tuwien.ac.at> wrote:
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                <div><div dir="ltr">I tried your struct file, converged with RKM=6, saved, increased RKMax <br clear="none">to 7 and continued with run_lapw.<br clear="none">No problem. As expected with your RMTs rather small change from 6 to 7 <br clear="none">and quick convergence.<br clear="none"><br clear="none">You must have changed something else, like mixing a density with <br clear="none">different RMTs, .... ????<br clear="none"><br clear="none"><br clear="none">Am 12.11.2023 um 07:30 schrieb hajar.nejatipoor--- via Wien:<br clear="none">> Dear Dr. Blaha<br clear="none">> The way you proposed, just worked for RKm=6, and the error below <br clear="none">> appeared for the case of RKm=7:<br clear="none">>   'SELECT' - no energy limits found for atom   1  L= 0<br clear="none">>   'SELECT' - E-bottom -520.00000   E-top -520.00000<br clear="none">> <br clear="none">> It is worth to mention that since for Si-muffin tin radius 1.68, there <br clear="none">> is a huge charge leak out, I set the muffin tin raddii as:<br clear="none">> <br clear="none">>    1  42.0  2.12  2.2<br clear="none">>    2  14.0  1.68  2.1<br clear="none">>    3  7.0  1.61  1.2<br clear="none">>    4  7.0  1.60  1.2<br clear="none">> <br clear="none">> On Saturday, November 11, 2023 at 10:43:42 PM GMT+3:30, Peter Blaha <br clear="none">> <<a shape="rect" ymailto="mailto:peter.blaha@tuwien.ac.at" href="mailto:peter.blaha@tuwien.ac.at">peter.blaha@tuwien.ac.at</a>> wrote:<br clear="none">> <br clear="none">> <br clear="none">> First of all,  setrmt  gives:<br clear="none">>    1  42.0  2.12  2.12<br clear="none">>    2  14.0  1.68  1.68<br clear="none">>    3  7.0  1.61  1.60<br clear="none">>    4  7.0  1.60  1.60<br clear="none">> <br clear="none">> So the N radii are much larger and Si and Mo smaller.<br clear="none">> <br clear="none">> It might be that the ghostband comes from N-2s, as the small RMT may not<br clear="none">> allow for 2 radial functions. You could try to remove the LO for N-s<br clear="none">> (only keep:<br clear="none">>    0.30    2  0      (GLOBAL E-PARAMETER WITH n OTHER CHOICES, global<br clear="none">> APW/LAPW)<br clear="none">>    0  -1.07    0.0010 CONT 1<br clear="none">>    1    0.30    0.0000 CONT 1<br clear="none">> for the N atoms (maybe use instead a HDLO).<br clear="none">> <br clear="none">> <br clear="none">> Am 11.11.2023 um 19:26 schrieb hajar.nejatipoor--- via Wien:<br clear="none">>  > MoSi2N4<br clear="none">>  > H   LATTICE,NONEQUIV.ATOMS:  4 187_P-6m2<br clear="none">>  > MODE OF CALC=RELA unit=bohr<br clear="none">>  >    5.502431  5.502431 38.534460 90.000000 90.000000120.000000<br clear="none">>  > ATOM  -1: X=0.00000000 Y=0.00000000 Z=0.00000000<br clear="none">>  >            MULT= 1          ISPLIT= 4<br clear="none">>  > Mo1        NPT=  781  R0=0.00001000 RMT=    2.2000   Z: 42.000<br clear="none">>  > LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000<br clear="none">>  >                       0.0000000 1.0000000 0.0000000<br clear="none">>  >                       0.0000000 0.0000000 1.0000000<br clear="none">>  > ATOM  -2: X=0.66666666 Y=0.33333334 Z=0.14710600<br clear="none">>  >            MULT= 2          ISPLIT= 4<br clear="none">>  >        -2: X=0.66666668 Y=0.33333334 Z=0.85289400<br clear="none">>  > Si1        NPT=  781  R0=0.00010000 RMT=    2.1000   Z: 14.000<br clear="none">>  > LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000<br clear="none">>  >                       0.0000000 1.0000000 0.0000000<br clear="none">>  >                       0.0000000 0.0000000 1.0000000<br clear="none">>  > ATOM  -3: X=0.33333333 Y=0.66666667 Z=0.82807700<br clear="none">>  >            MULT= 2          ISPLIT= 4<br clear="none">>  >        -3: X=0.33333334 Y=0.66666667 Z=0.17192300<br clear="none">>  > N 1        NPT=  781  R0=0.00010000 RMT=    1.2000   Z:  7.000<br clear="none">>  > LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000<br clear="none">>  >                       0.0000000 1.0000000 0.0000000<br clear="none">>  >                       0.0000000 0.0000000 1.0000000<br clear="none">>  > ATOM  -4: X=0.66666666 Y=0.33333334 Z=0.93855400<br clear="none">>  >            MULT= 2          ISPLIT= 4<br clear="none">>  >        -4: X=0.66666668 Y=0.33333334 Z=0.06144600<br clear="none">>  > N 2        NPT=  781  R0=0.00010000 RMT=    1.2000   Z:  7.000<br clear="none">>  > LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000<br clear="none">>  >                       0.0000000 1.0000000 0.0000000<br clear="none">>  >                       0.0000000 0.0000000 1.0000000<br clear="none">> <br clear="none">> -- <br clear="none">> --------------------------------------------------------------------------<br clear="none">> Peter BLAHA, Inst.f. Materials Chemistry, TU Vienna, A-1060 Vienna<br clear="none">> Phone: +43-1-58801-165300<br clear="none">> Email: <a shape="rect" ymailto="mailto:peter.blaha@tuwien.ac.at" href="mailto:peter.blaha@tuwien.ac.at">peter.blaha@tuwien.ac.at</a> <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