Hello all,

I tried to calculate the electronic structure of FeO using mBJ.

1. I took the cubic FeO structure, made a 2x2x2 primitive supercell, relabeled the Fe sites "1" and "2" to get the appropriate AFM ordering, ran sgroup, and obtained a rhombohedral cell with 2 Fe sites and 1 O site. This structure looks correct when viewed with VESTA or xcrysden, so I think I am using the correct structure.

2. I run a spin-polarized PBE calculation, initializing the Fe to "up" and "down", and the O to "no spin", this converges quickly and obtains a zero band gap as expected.

3. I run an mBJ calculation using PRATT mixing, slowly increasing the mixing factor. The energy converges in 20 cycles or so, however the charge never converges - it keeps "sloshing" back and forth between the two Fe sites. The band gap for this system remains at zero.

In PRL 102 226401 (2009) and mBJ calculation on FeO reports a gap of 1.82 eV. May I ask Dr. Fabian Tran and/or Dr. Peter Blaha, to obtain these results did you:
   1. Perform an AFM calculation or just a spin-polarized calculation?
   2. Perform any sort of structural optimization?
   3. Use PRATT mixing only, or switch back to MSR1?

I also tried this approach with hematite (Fe2O3), obtaining a rhombohedral structure with 4 inequivalent Fe sites (as expected), and following the same steps I obtained good charge and energy convergence in mBJ as well as a reasonably accurate band gap - so I find it a bit curious that my approach fails for FeO.

I would greatly appreciate a quick tip on how the original calculations in PRL 102 226401 were performed.

John McLeod

Wien mailing list

Reply via email to