Determining the Magnetic Anisotropy: Difference between revisions
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Description: Magnetocrystalline Anisotropy Energy | Description: Magnetocrystalline Anisotropy Energy determined non-self-consistently | ||
---- | The Magnetocrystalline Anisotropy Energy is determined by rotating all spins according to different directions. First of all, an accurate ([[PREC|PREC]] = Accurate, [[LREAL|LREAL]] = .False.) collinear calculation (using the <tt>vasp_std</tt> version) in the ground state has to be done. Next, the spin-orbit coupling ([[LSORBIT|LSORBIT]] = .True. using the <tt>vasp_ncl</tt> version) is taken into account non-self-consistently ([[ICHARG|ICHARG]] = 11) for several spin orientations. In most cases, the changes in energies are very low (sometimes around micro-eV). The number of bands for the has to be doubled compared to the collinear run. | ||
< | To modify the orientation of the spins in the crystal, we consider the second approach described [[SAXIS|here]]. For the [[MAGMOM|MAGMOM]]-tag, the total local magnetic moment is written according to the z-direction (necessarily, the x and y-directions are equal to 0). The spin orientation <math>(u,v,w)</math> is defined by the [[SAXIS|SAXIS]]-tag in the Cartesian frame. The Magnetocrystalline Anisotropy Energy is calculated by orientating the spins in different directions and the following equation | ||
::<math>E_{\text{MAE}} = E_{(u,v,w)} - E_0</math> | |||
with <math>E_0</math> the energy of the most stable spin orientation. | |||
More details are available in the [[SAXIS|SAXIS]] and [[LSORBIT|LSORBIT]] pages. | |||
''<u>Exercise :</u>'' Determine the Magnetocrystalline Anisotropy Energy of NiO in a non self-consistent approach by orientating the spins along the following path : (2,2,2) --> (2,2,1) --> (2,2,0) --> ... --> (2,2,-6). Compare to the [[Including_the_Spin-Orbit_Coupling|self-consistent approach]]. | |||
---- | |||
*{{TAG|INCAR}} | |||
GGA+U | NiO MAE | ||
{{TAGBL|SYSTEM}} = "NiO" | |||
Electronic minimization | |||
{{TAGBL|PREC}} = Accurate | |||
{{TAGBL|ENCUT}} = 450 | |||
{{TAGBL|EDIFF}} = 1E-7 | |||
{{TAGBL|LORBIT}} = 11 | |||
{{TAGBL|LREAL}} = .False. | |||
{{TAGBL|ISYM}} = -1 | |||
{{TAGBL|NELMIN}} = 6 | |||
# {{TAGBL|ICHARG}} = 11 | |||
# {{TAGBL|LCHARG}} = .FALSE. | |||
# {{TAGBL|LWAVE}} = .FALSE. | |||
# {{TAGBL|NBANDS}} = 52 | |||
# {{TAGBL|GGA_COMPAT}} = .FALSE. | |||
DOS | |||
{{TAGBL|ISMEAR}} = -5 | |||
Magnetism | |||
{{TAGBL|ISPIN}} = 2 | |||
{{TAGBL|MAGMOM}} = 2.0 -2.0 2*0.0 | |||
# {{TAGBL|MAGMOM}} = 0 0 2 0 0 -2 6*0 # Including Spin-orbit | |||
# {{TAGBL|LSORBIT}} = .True. | |||
# {{TAGBL|SAXIS}} = 1 0 0 # Quantization axis used to rotate all spins in a direction defined in the (O,x,y,z) Cartesian frame | |||
Orbital mom. | |||
{{TAGBL|LORBMOM}} = T | |||
Mixer | |||
{{TAGBL|AMIX}} = 0.2 | |||
{{TAGBL|BMIX}} = 0.00001 | |||
{{TAGBL|AMIX_MAG}} = 0.8 | |||
{{TAGBL|BMIX_MAG}} = 0.00001 | |||
GGA+U | |||
{{TAGBL|LDAU}} = .TRUE. | |||
{{TAGBL|LDAUTYPE}} = 2 | |||
{{TAGBL|LDAUL}} = 2 -1 | |||
{{TAGBL|LDAUU}} = 5.00 0.00 | |||
{{TAGBL|LDAUJ}} = 0.00 0.00 | |||
{{TAGBL|LDAUPRINT}} = 1 | |||
{{TAGBL|LMAXMIX}} = 4 | |||
*KPOINTS | *{{TAG|KPOINTS}} | ||
<pre> | <pre> | ||
k-points | k-points | ||
Line 56: | Line 69: | ||
</pre> | </pre> | ||
*POSCAR | *{{TAG|POSCAR}} | ||
<pre> | <pre> | ||
NiO | NiO | ||
Line 70: | Line 83: | ||
1.5 1.5 1.5 | 1.5 1.5 1.5 | ||
</pre> | </pre> | ||
== Download == | == Download == | ||
[ | [[Media:nio_noSOC.tgz| nio_noSOC.tgz]] | ||
---- | ---- | ||
[[Category:Examples]] | [[Category:Examples]] |
Latest revision as of 08:48, 11 April 2023
Description: Magnetocrystalline Anisotropy Energy determined non-self-consistently
The Magnetocrystalline Anisotropy Energy is determined by rotating all spins according to different directions. First of all, an accurate (PREC = Accurate, LREAL = .False.) collinear calculation (using the vasp_std version) in the ground state has to be done. Next, the spin-orbit coupling (LSORBIT = .True. using the vasp_ncl version) is taken into account non-self-consistently (ICHARG = 11) for several spin orientations. In most cases, the changes in energies are very low (sometimes around micro-eV). The number of bands for the has to be doubled compared to the collinear run.
To modify the orientation of the spins in the crystal, we consider the second approach described here. For the MAGMOM-tag, the total local magnetic moment is written according to the z-direction (necessarily, the x and y-directions are equal to 0). The spin orientation is defined by the SAXIS-tag in the Cartesian frame. The Magnetocrystalline Anisotropy Energy is calculated by orientating the spins in different directions and the following equation
with the energy of the most stable spin orientation. More details are available in the SAXIS and LSORBIT pages.
Exercise : Determine the Magnetocrystalline Anisotropy Energy of NiO in a non self-consistent approach by orientating the spins along the following path : (2,2,2) --> (2,2,1) --> (2,2,0) --> ... --> (2,2,-6). Compare to the self-consistent approach.
NiO MAE SYSTEM = "NiO" Electronic minimization PREC = Accurate ENCUT = 450 EDIFF = 1E-7 LORBIT = 11 LREAL = .False. ISYM = -1 NELMIN = 6 # ICHARG = 11 # LCHARG = .FALSE. # LWAVE = .FALSE. # NBANDS = 52 # GGA_COMPAT = .FALSE. DOS ISMEAR = -5 Magnetism ISPIN = 2 MAGMOM = 2.0 -2.0 2*0.0 # MAGMOM = 0 0 2 0 0 -2 6*0 # Including Spin-orbit # LSORBIT = .True. # SAXIS = 1 0 0 # Quantization axis used to rotate all spins in a direction defined in the (O,x,y,z) Cartesian frame Orbital mom. LORBMOM = T Mixer AMIX = 0.2 BMIX = 0.00001 AMIX_MAG = 0.8 BMIX_MAG = 0.00001 GGA+U LDAU = .TRUE. LDAUTYPE = 2 LDAUL = 2 -1 LDAUU = 5.00 0.00 LDAUJ = 0.00 0.00 LDAUPRINT = 1 LMAXMIX = 4
k-points 0 gamma 4 4 4 0 0 0
NiO 4.17 1.0 0.5 0.5 0.5 1.0 0.5 0.5 0.5 1.0 2 2 Cartesian 0.0 0.0 0.0 1.0 1.0 1.0 0.5 0.5 0.5 1.5 1.5 1.5