LSCK: Difference between revisions
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{{sc|LSCK|Examples|Examples that use this tag}} | {{sc|LSCK|Examples|Examples that use this tag}} | ||
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[[Category:INCAR]][[Category:Many-Body Perturbation Theory]][[Category:GW]][[Category:ACFDT]] | [[Category:INCAR tag]][[Category:Many-Body Perturbation Theory]][[Category:GW]][[Category:ACFDT]] |
Revision as of 14:41, 8 April 2022
LSCK = [logical]
Default: LSCK = .FALSE.
Description: LSCK=True switches on the use of 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