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]:
This kernel 'squeezes' the contributions from large wave vectors into the window given by ENCUTGWSOFT. Effectively, this extrapolates the random-phase-approximation–correlation energy to the ENCUTGW limit, assuming that the basis-set-incompleteness error falls off as ENCUTGW.
Related tags and articles
ENCUTGW, GW calculations ACFDT/RPA calculations