LSCK: Difference between revisions

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{{TAGDEF|LSCK|[logical]| .FALSE.}}    
{{TAGDEF|LSCK|[logical]| .FALSE.}}                          
Up to vasp.6.2, the default was LSCK = .TRUE.
{{NB|important|Up to vasp.6.2, the default was {{TAG|LSCK}}{{=}} .TRUE.}}
----Description: {{TAG|LSCK}}=.True. switches on the squeezed Coulomb kernel.
----Description: {{TAG|LSCK}}=.True. switches on the squeezed Coulomb kernel.
If {{TAG|LSCK}} is set to .TRUE., the squeezed Coulomb kernel is used instead of the [[ENCUTGWSOFT|cosine window]] {{cite|riemelmoser:jcp:2020}}:
If {{TAG|LSCK}} is set to .TRUE., the squeezed Coulomb kernel is used instead of the [[ENCUTGWSOFT|cosine window]] {{cite|riemelmoser:jcp:2020}}:

Latest revision as of 08:41, 29 August 2024

LSCK = [logical]
Default: LSCK = .FALSE. 

Important: Up to vasp.6.2, the default was LSCK= .TRUE.

Description: LSCK=.True. switches on the squeezed Coulomb kernel.

If LSCK is set to .TRUE., the squeezed Coulomb kernel is used instead of the cosine window [1]:

[math]\displaystyle{ v_{G} = 4 \pi e^2 \frac{ (G_{max}-G_{min})(G_{max}-G) }{ (G_{min}^2 - G(2G_{min}-G_{max}))^2 } \qquad \mbox{for} \quad \mathrm{ENCUTGWSOFT}=\frac{\hbar^2G_{min}^2}{2m_e}\lt \frac{\hbar^2 G^2}{2m_e}\lt \frac{\hbar^2G_{max}^2}{2m_e}=\mathrm{ENCUTGW} }[/math]

This kernel 'squeezes' the contributions from large wave vectors [math]\displaystyle{ G\gt G_{max} }[/math] into the window given by ENCUTGWSOFT. Effectively, this extrapolates the random-phase-approximation–correlation energy to the ENCUTGW [math]\displaystyle{ \to \infty }[/math] limit, assuming that the basis-set-incompleteness error falls off as [math]\displaystyle{ 1/ }[/math]ENCUTGW[math]\displaystyle{ ^{3/2} }[/math].

Related tags and articles

ENCUTGW, GW calculations ACFDT/RPA calculations

Examples that use this tag