LCALCPOL: Difference between revisions
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For {{TAG|LCALCPOL}}=.TRUE., VASP calculates the electronic contribution to the polarization, along the three reciprocal lattice vectors '''G'''<sub>i</sub>, i=1,2,3, (i.e. Σ<sub>i</sub> '''P'''·'''G'''<sub>i</sub>) in a single run (unlike {{TAG|LBERRY}}=.TRUE.). | For {{TAG|LCALCPOL}}=.TRUE., VASP calculates the electronic contribution to the polarization, along the three reciprocal lattice vectors '''G'''<sub>i</sub>, i=1,2,3, (i.e. Σ<sub>i</sub> '''P'''·'''G'''<sub>i</sub>) in a single run (unlike {{TAG|LBERRY}}=.TRUE.). | ||
An example: | === An example: The fluorine displacement dipole (Born effective charge) in NaF === | ||
*With {{FILE|INCAR}} file: | *With {{FILE|INCAR}} file: | ||
PREC = Med | {{TAGBL|PREC}} = Med | ||
EDIFF= 1E-6 | {{TAGBL|EDIFF}}= 1E-6 | ||
ISMEAR = 0 | {{TAGBL|ISMEAR}} = 0 | ||
DIPOL = 0.25 0.25 0.25 | {{TAGBL|DIPOL}} = 0.25 0.25 0.25 | ||
LCALCPOL = .TRUE. | {{TAGBL|LCALCPOL}} = .TRUE. | ||
*{{FILE|KPOINTS}} file: | *{{FILE|KPOINTS}} file: | ||
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Total electronic dipole moment: p[elc]=( 0.00000 0.00000 0.00000 ) electrons Angst | Total electronic dipole moment: p[elc]=( 0.00000 0.00000 0.00000 ) electrons Angst | ||
Here the units "electrons Angst" denote <math>e\AA=-1.602 10^{-19}C\AA</math>. | |||
To calculate the change in the electronic polarization of NaF due to the displacement of the fluorine sublattice we repeat the previous calculation with the following {{FILE|POSCAR}} file: | To calculate the change in the electronic polarization of NaF due to the displacement of the fluorine sublattice we repeat the previous calculation with the following {{FILE|POSCAR}} file: | ||
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<math>\Delta\mathrm{p[tot]}=0.36061-0.31571=0.0449\hat{z}\;e\AA</math> | <math>\Delta\mathrm{p[tot]}=0.36061-0.31571=0.0449\hat{z}\;e\AA</math> | ||
and considering that the F-sublattice was displaced by 0.045102 Å these calculations yield a Born effective charge for fluorine of | and considering that the F-sublattice was displaced by 0.045102 Å these calculations yield a Born effective charge for fluorine of | ||
== Related | <math>Z^*=0.0449/0.045102=-0.995|e|\;</math>. | ||
The socalled parallel or <math>\bold{G}_{\parallel}</math> | |||
direction in the integration over the reciprocal space unit cell is set in {{TAG|IGPAR}}. | |||
== Related tags and articles == | |||
{{TAG|LCALCEPS}}, | {{TAG|LCALCEPS}}, | ||
{{TAG|EFIELD_PEAD}}, | {{TAG|EFIELD_PEAD}}, | ||
Line 87: | Line 93: | ||
{{TAG|DIPOL}}, | {{TAG|DIPOL}}, | ||
[[Berry_phases_and_finite_electric_fields|Berry phases and finite electric fields]] | [[Berry_phases_and_finite_electric_fields|Berry phases and finite electric fields]] | ||
{{sc|LCALCPOL|Examples|Examples that use this tag}} | |||
---- | ---- | ||
[[Category:INCAR]][[Category:Berry phases]] | [[Category:INCAR tag]][[Category:Linear response]][[Category:Dielectric properties]][[Category:Berry phases]] |
Latest revision as of 07:58, 19 July 2022
LCALCPOL = .TRUE. | .FALSE.
Default: LCALCPOL = .FALSE.
Description: LCALCPOL=.TRUE. switches on the evaluation of the Berry phase expressions for the macroscopic electronic polarization in accordance with the so-called Modern Theory of Polarization.
For LCALCPOL=.TRUE., VASP calculates the electronic contribution to the polarization, along the three reciprocal lattice vectors Gi, i=1,2,3, (i.e. Σi P·Gi) in a single run (unlike LBERRY=.TRUE.).
An example: The fluorine displacement dipole (Born effective charge) in NaF
- With INCAR file:
PREC = Med EDIFF= 1E-6 ISMEAR = 0 DIPOL = 0.25 0.25 0.25 LCALCPOL = .TRUE.
- KPOINTS file:
6x6x6 0 Gamma 6 6 6 0 0 0
- POSCAR file:
NaF 4.5102 0.0 0.5 0.5 0.5 0.0 0.5 0.5 0.5 0.0 1 1 Direct 0.0000000000000000 0.0000000000000000 0.0000000000000000 0.5000000000000000 0.5000000000000000 0.5000000000000000
- and LDA Na_sv and F PAW datasets.
The OUTCAR file should now contain the following lines:
Ionic dipole moment: p[ion]=( 2.25510 2.25510 2.25510 ) electrons Angst Total electronic dipole moment: p[elc]=( 0.00000 0.00000 0.00000 ) electrons Angst
Here the units "electrons Angst" denote .
To calculate the change in the electronic polarization of NaF due to the displacement of the fluorine sublattice we repeat the previous calculation with the following POSCAR file:
NaF 4.5102 0.0 0.5 0.5 0.5 0.0 0.5 0.5 0.5 0.0 1 1 Direct 0.0000000000000000 0.0000000000000000 0.0000000000000000 0.5100000000000000 0.5100000000000000 0.4900000000000000
The OUTCAR should now contain something very similar to the following lines:
Ionic dipole moment: p[ion]=( 2.25510 2.25510 1.93939 ) electrons Angst Total electronic dipole moment: p[elc]=( 0.00000 0.00000 0.36061 ) electrons Angst
From the above one easily recognizes that the change in the electronic dipole moment due to the F-sublattice displacement is:
and the corresponding change in the ionic dipole moment:
Thus the total change is found to be:
and considering that the F-sublattice was displaced by 0.045102 Å these calculations yield a Born effective charge for fluorine of
.
The socalled parallel or direction in the integration over the reciprocal space unit cell is set in IGPAR.
Related tags and articles
LCALCEPS, EFIELD_PEAD, LPEAD, IPEAD, LBERRY, IGPAR, NPPSTR, DIPOL, Berry phases and finite electric fields