Check symmetry breaking under influence of SOI and/or electric charge |
- Date: 2022/03/26 13:09
- Name: Bagus
<bagusnuryasin_3225160838@mhs.unj.ac.id>
- Dear OpenMX users,
I would like to examine symmetry breaking under the influence of SOC and/or electric field to confirm band splitting and/or band structure shifting. However, after doing the calculations, there is no change in atomic distance Ni-Br or atomic angle Ni-Br-Ni when I visualize the .xyz and .bulk.xyz output files on VESTA.
how to check that symmetry break? any input errors in the .dat file? any recommendations to confirm band splitting and/or band structure shifting?
here's my .dat file
### (base) non-collinear NiBr2 monolayer without SOC and electric field # # Definition of Atomic Species # Species.Number 2 <Definition.of.Atomic.Species Br Br7.0-s3p3d2 Br_PBE19 Ni Ni6.0S-s3p3d2f1 Ni_PBE19S Definition.of.Atomic.Species>
# # Atoms # Atoms.Number 3 Atoms.SpeciesAndCoordinates.Unit FRAC # Ang|AU <Atoms.SpeciesAndCoordinates 1 Ni 0.00000000000000 0.00000000000000 0.00000000000000 10.0 6.0 0.0 0.0 0.0 0.0 0 off 2 Br 0.33364644113299 0.66610406570644 0.08017052963226 3.5 3.5 0.0 0.0 0.0 0.0 0 off 3 Br 0.66635356275338 0.33389594190917 0.91982946734286 3.5 3.5 0.0 0.0 0.0 0.0 0 off Atoms.SpeciesAndCoordinates>
Atoms.UnitVectors.Unit Ang <Atoms.UnitVectors 3.700000000000000 0.000000000000000 0.000000000000000 -1.850000000000000 3.204294000000000 0.000000000000000 0.000000000000000 0.000000000000000 17.260000228900001 Atoms.UnitVectors>
# # SCF or Electronic System # scf.electric.field 0.0 0.0 0.0 # default=0.0 scf.XcType GGA-PBE # LDA|LSDA-CA|LSDA-PW|GGA-PBE scf.SpinPolarization NC # On|Off|NC scf.ElectronicTemperature 300 # default=300 (K) scf.energycutoff 300 # default=150 (Ry) scf.maxIter 300 # default=40 scf.EigenvalueSolver band # DC|GDC|Cluster|Band scf.Kgrid 16 16 1 # means n1 x n2 x n3 scf.Mixing.Type rmm-diish # Simple|Rmm-Diis|Gr-Pulay|Kerker|Rmm-Diisk scf.Init.Mixing.Weight 0.01 # default=0.30 scf.Min.Mixing.Weight 0.001 # default=0.001 scf.Max.Mixing.Weight 0.01 # default=0.40 scf.Mixing.History 40 # default=5 scf.Mixing.StartPulay 30 # default=6 scf.criterion 1.0e-8 # default=1.0e-6 (Hartree) scf.spinorbit.coupling off
# # MD or Geometry Optimization # MD.Type Nomd # Nomd|Opt|NVE|NVT_VS|NVT_NH MD.maxIter 30 # default=1 MD.Opt.DIIS.History 3O MD.Opt.StartDIIS 5 MD.Opt.EveryDIIS 200 #MD.TimeStep 1 # default=0.5 (fs) MD.Opt.criterion 1.0e-4 # default=1.0e-4 (Hartree/bohr)
<MD.Fixed.XYZ 1 1 1 1 2 0 0 0 3 0 0 0 MD.Fixed.XYZ>
# # Band dispersion # Band.dispersion on # on|off, default=off # if <Band.KPath.UnitCell does not exist, # the reciprical lattice vector is employed. Band.Nkpath 3 <Band.kpath 200 0.5 0.0 0.0 0.0 0.0 0.0 M g 200 0.0 0.0 0.0 0.67777 -0.33333 0.0 g K 200 0.677777 -0.33333 0.0 0.5 0.0 0.0 K M Band.kpath>
### non-collinear NiBr2 monolayer with SOC effect and without electric field # # Definition of Atomic Species # Species.Number 2 <Definition.of.Atomic.Species Br Br7.0-s3p3d2 Br_PBE19 Ni Ni6.0S-s3p3d2f1 Ni_PBE19S Definition.of.Atomic.Species>
# # Atoms # Atoms.Number 3 Atoms.SpeciesAndCoordinates.Unit FRAC # Ang|AU <Atoms.SpeciesAndCoordinates 1 Ni 0.00000000000000 0.00000000000000 0.00000000000000 10.0 6.0 0.0 0.0 0.0 0.0 0 off 2 Br 0.33364644113299 0.66610406570644 0.08017052963226 3.5 3.5 0.0 0.0 0.0 0.0 0 off 3 Br 0.66635356275338 0.33389594190917 0.91982946734286 3.5 3.5 0.0 0.0 0.0 0.0 0 off Atoms.SpeciesAndCoordinates>
Atoms.UnitVectors.Unit Ang <Atoms.UnitVectors 3.700000000000000 0.000000000000000 0.000000000000000 -1.850000000000000 3.204294000000000 0.000000000000000 0.000000000000000 0.000000000000000 17.260000228900001 Atoms.UnitVectors>
# # SCF or Electronic System # scf.electric.field 0.0 0.0 0.0 # default=0.0 scf.XcType GGA-PBE # LDA|LSDA-CA|LSDA-PW|GGA-PBE scf.SpinPolarization NC # On|Off|NC scf.ElectronicTemperature 300 # default=300 (K) scf.energycutoff 300 # default=150 (Ry) scf.maxIter 300 # default=40 scf.EigenvalueSolver band # DC|GDC|Cluster|Band scf.Kgrid 16 16 1 # means n1 x n2 x n3 scf.Mixing.Type rmm-diish # Simple|Rmm-Diis|Gr-Pulay|Kerker|Rmm-Diisk scf.Init.Mixing.Weight 0.01 # default=0.30 scf.Min.Mixing.Weight 0.001 # default=0.001 scf.Max.Mixing.Weight 0.01 # default=0.40 scf.Mixing.History 40 # default=5 scf.Mixing.StartPulay 30 # default=6 scf.criterion 1.0e-8 # default=1.0e-6 (Hartree) scf.spinorbit.coupling on scf.restart on # on|off,default=off
# # MD or Geometry Optimization # MD.Type Nomd # Nomd|Opt|NVE|NVT_VS|NVT_NH MD.maxIter 30 # default=1 MD.Opt.DIIS.History 3O MD.Opt.StartDIIS 5 MD.Opt.EveryDIIS 200 #MD.TimeStep 1 # default=0.5 (fs) MD.Opt.criterion 1.0e-4 # default=1.0e-4 (Hartree/bohr)
<MD.Fixed.XYZ 1 1 1 1 2 0 0 0 3 0 0 0 MD.Fixed.XYZ>
# # Band dispersion # Band.dispersion on # on|off, default=off # if <Band.KPath.UnitCell does not exist, # the reciprical lattice vector is employed. Band.Nkpath 3 <Band.kpath 200 0.5 0.0 0.0 0.0 0.0 0.0 M g 200 0.0 0.0 0.0 0.67777 -0.33333 0.0 g K 200 0.677777 -0.33333 0.0 0.5 0.0 0.0 K M Band.kpath>
### non-collinear NiBr2 monolayer with 25 GV/m electric field and without SOC effect # # Definition of Atomic Species # Species.Number 2 <Definition.of.Atomic.Species Br Br7.0-s3p3d2 Br_PBE19 Ni Ni6.0S-s3p3d2f1 Ni_PBE19S Definition.of.Atomic.Species>
# # Atoms # Atoms.Number 3 Atoms.SpeciesAndCoordinates.Unit FRAC # Ang|AU <Atoms.SpeciesAndCoordinates 1 Ni 0.00000000000000 0.00000000000000 0.00000000000000 10.0 6.0 0.0 0.0 0.0 0.0 0 off 2 Br 0.33364644113299 0.66610406570644 0.08017052963226 3.5 3.5 0.0 0.0 0.0 0.0 0 off 3 Br 0.66635356275338 0.33389594190917 0.91982946734286 3.5 3.5 0.0 0.0 0.0 0.0 0 off Atoms.SpeciesAndCoordinates>
Atoms.UnitVectors.Unit Ang <Atoms.UnitVectors 3.700000000000000 0.000000000000000 0.000000000000000 -1.850000000000000 3.204294000000000 0.000000000000000 0.000000000000000 0.000000000000000 17.260000228900001 Atoms.UnitVectors>
# # SCF or Electronic System # scf.electric.field 0.0 0.0 25.0 # default=0.0 scf.XcType GGA-PBE # LDA|LSDA-CA|LSDA-PW|GGA-PBE scf.SpinPolarization NC # On|Off|NC scf.ElectronicTemperature 300 # default=300 (K) scf.energycutoff 300 # default=150 (Ry) scf.maxIter 300 # default=40 scf.EigenvalueSolver band # DC|GDC|Cluster|Band scf.Kgrid 16 16 1 # means n1 x n2 x n3 scf.Mixing.Type rmm-diis # Simple|Rmm-Diis|Gr-Pulay|Kerker|Rmm-Diisk scf.Init.Mixing.Weight 0.01 # default=0.30 scf.Min.Mixing.Weight 0.001 # default=0.001 scf.Max.Mixing.Weight 0.01 # default=0.40 scf.Mixing.History 40 # default=5 scf.Mixing.StartPulay 30 # default=6 scf.criterion 1.0e-8 # default=1.0e-6 (Hartree) scf.spinorbit.coupling off
# # MD or Geometry Optimization # MD.Type Nomd # Nomd|Opt|NVE|NVT_VS|NVT_NH MD.maxIter 30 # default=1 MD.Opt.DIIS.History 3O MD.Opt.StartDIIS 5 MD.Opt.EveryDIIS 200 #MD.TimeStep 1 # default=0.5 (fs) MD.Opt.criterion 1.0e-4 # default=1.0e-4 (Hartree/bohr)
<MD.Fixed.XYZ 1 1 1 1 2 0 0 0 3 0 0 0 MD.Fixed.XYZ>
# # Band dispersion # Band.dispersion on # on|off, default=off # if <Band.KPath.UnitCell does not exist, # the reciprical lattice vector is employed. Band.Nkpath 3 <Band.kpath 200 0.5 0.0 0.0 0.0 0.0 0.0 M g 200 0.0 0.0 0.0 0.67777 -0.33333 0.0 g K 200 0.677777 -0.33333 0.0 0.5 0.0 0.0 K M Band.kpath>
Thank you very much.
Best regards,
Bagus
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