SYSTEM = Fe3O4 + FA NCORE = 8 ENCUT = 520 # energy cut-off in eV PREC = Accurate # accurate precision LREAL = .FALSE. # .FALSE. is necessary for accurate peak intensities ISMEAR = 0 # Gaussian smearing SIGMA = 0.05 # parameter for Gaussian smearing NSW = 1 # no relaxation, only vibrational analysis NELMIN = 10 # min. number of electronic steps NELM = 500 # max. number of electronic steps NELMDL = -12 # delay for self-consistent steps EDIFF = 2E-8 # break condition for electronic loop NFREE = 2 # include positive and negative displacements GGA = PE # GGA with xc functional PBE ISPIN = 2 # spin polarized calculation LORBIT = 11 # calculate local magnetic moments MAGMOM = N(Fe_tet)*-5.0 N(Fe_oct)*5.0 N(others(O,H,C))*0.0 # initial magnetic moments LDAU = .TRUE. # +U calculation LDAUTYPE = 2 # simplified approach by Dudarev et al. LDAUL = 2 -1 -1 -1 # add on-site potential only to the d-orbitals of Fe (1st species in POSCAR, 1st value in this list equals 2) and no on-site potential for other species (2nd to 4th species in POSCAR and this list, value equals -1) LDAUU = 4.0 0.0 0.0 0.0 # Ueff = 4.0 eV for Fe and 0.0 eV for O, C, H LDAUJ = 0.0 0.0 0.0 0.0 # for LDAUTYPE = 2 only U-J is meaningfull -> set J=0 LDAUPRINT = 0 # don't write occupancy matrix to OUTCAR LASPH = .TRUE. # take aspherical charge distribution into account LMAXMIX = 4 # take d-orbitals into account in the charge density mixer #AMIX = 0.2 # recommended #BMIX = 0.00001 # mixing parameters #AMIX_MAG = 0.8 # in case of #BMIX_MAG = 0.00001 # slow convergence IDIPOL = 3 # dipole along c-axis LDIPOL = .TRUE. # include dipole corrections DIPOL = CM_x CM_y CM_z # center of mass in fractional coordinates IBRION = 7 # DFPT calculation LEPSILON = .TRUE. # enables Born effective charges (BEC) tensors NWRITE = 3 # sqrt(mass)-devided eigenvectors in OUTCAR POTIM = 0.02 # ISYM = 0 # switch off symmetry (recommended)