Your :MMI and the :MMT look absolutely ok.
The Lu are basically non-magnetic, the O seem to behave antiferromagnetically. It means you should have the same number of spin-up and dn electrons, i.e. you have the same occupations and thus should have a gap in both spin-directions.

Maybe you need to converge the scf cycle better (smaller :DIS)

After that, if you still have a half-metal, analyse the partial DOS and the band structures to find out which states are at EF.
In case of Lu-f, you may need a U also on Lu-4f.




Am 05.03.2020 um 08:37 schrieb Ali Baghizhadeh:
Dear Prof. Blaha

Thank you.

In hexagonal structure, LuFeO3 has 6 f.u. per unit cell with 30 atoms. Once I split Fe (6c Wyckoff) to Fe1 and Fe2, it changes space group to the one with lower symmetry and I am trying to even lower symmetry by splitting at least oxygen atoms. The final objective is core hole for EELS calculations, so I do not want multiplicity of atoms.

The analysis of case.scf shows following results:

MMT: 0.00012

MMI:

case.scf::MMI001: MAGNETIC MOMENT IN SPHERE   1    =   -0.00350

case.scf::MMI002: MAGNETIC MOMENT IN SPHERE   2    =   -0.00613

case.scf::MMI003: MAGNETIC MOMENT IN SPHERE   3    =   -0.00768

case.scf::MMI004: MAGNETIC MOMENT IN SPHERE   4    =   -0.00385

case.scf::MMI005: MAGNETIC MOMENT IN SPHERE   5    =    4.02712 (Fe)

case.scf::MMI006: MAGNETIC MOMENT IN SPHERE   6    =   -0.07328

case.scf::MMI007: MAGNETIC MOMENT IN SPHERE   7    =    0.09103

case.scf::MMI008: MAGNETIC MOMENT IN SPHERE   8    =   -0.09647

case.scf::MMI009: MAGNETIC MOMENT IN SPHERE   9    =    0.10131

case.scf::MMI010: MAGNETIC MOMENT IN SPHERE  10    =   -0.27719

case.scf::MMI011: MAGNETIC MOMENT IN SPHERE  11    =    0.26978

case.scf::MMI012: MAGNETIC MOMENT IN SPHERE  12    =   -0.28291

case.scf::MMI013: MAGNETIC MOMENT IN SPHERE  13    =    0.29177

case.scf::MMI014: MAGNETIC MOMENT IN SPHERE  14    =   -4.01690 (Fe)

Sincerely

Ali

------------------------------------------------------------------------

*From:*Wien <wien-boun...@zeus.theochem.tuwien.ac.at> on behalf of Peter Blaha <pbl...@theochem.tuwien.ac.at>
*Sent:* 04 March 2020 17:16
*To:* wien@zeus.theochem.tuwien.ac.at
*Subject:* Re: [Wien] LDA+U, spin up and down

LuFeO3 has 5 atoms per f.u. with one Fe.

You have 2 Fe atoms (5 and 14), thus I wonder how you manage to have at
least 14 different atoms per unit cell. Unless the Fe atoms have MULT=2
or higher, you can have at most 10 atoms/cell. So the question is: is
your stoichiometry correct ?

Also: What are the :MMI and :MMT ? Are the Lu non-magnetic ? Is :MMT~0

If spin-up .ne. spin-dn it means that some atoms are not AFM ordered
(even when the Fe are).



Am 04.03.2020 um 15:50 schrieb Ali Baghizhadeh:
Dear WIEN2k users

I am running spin polarized calculation on LuFeO3 structure, with Fe ions having spin up and down in unit cell. I did volume optimization/force minimization, and then I used LDA+U to open the bandgap. It does work fine for spin up when I plot the density of states, but for spin down, it is conductive. I cannot explain this behavior, and I do not know how to look for the root/s of the problem. Please any comment will be highly appreciated.

Case.inorb file: (Fe1 is atom 5 and Fe2 is atom 14)

1  2  0                     nmod, natorb, ipr

PRATT  1.0                    BROYD/PRATT, mixing

    5 1 2                          iatom nlorb, lorb

    14 1 2                          iatom nlorb, lorb

    1                              nsic 0..AMF, 1..SIC, 2..HFM

     0.367 0.073        U J (Ry)   Note: you can also use U_eff = U-J and J=0

     0.367 0.073        U J

Sincerely

Ali


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