LSCK: Difference between revisions

Revision as of 14:28, 20 December 2021

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]:

$v_{G}=4\pi e^{2}{\frac {(G_{max}-G_{min})(G_{max}-G)}{(G_{min}^{2}-G(2G_{min}-G_{max}))^{2}}}\qquad {\mbox{for}}\quad \mathrm {ENCUTGWSOFT} ={\frac {\hbar ^{2}G_{min}^{2}}{2m_{e}}}<{\frac {\hbar ^{2}G^{2}}{2m_{e}}}<{\frac {\hbar ^{2}G_{max}^{2}}{2m_{e}}}=\mathrm {ENCUTGW}$

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

Related Tags and Sections

ENCUTGW, GW calculations ACFDT/RPA calculations

Examples that use this tag

Contents

↑ S. Riemelmoser, M. Kaltak, and G. Kresse, JCP 152(13), 134103 (2020).

[riemelmoser:jcp:2020-1] S. Riemelmoser, M. Kaltak, and G. Kresse, JCP 152(13), 134103 (2020).

[1]

@@ Line 1: / Line 1: @@
 {{TAGDEF|LSCK|[logical]| .FALSE.}}
+Description: {{TAG|LSCK}}=True switches on the use of 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}}:
 <math>v_{G} = 4 \pi e^2 \frac{
@@ Line 10: / Line 12: @@
 \qquad \mbox{for} \quad  \mathrm{ENCUTGWSOFT}=\frac{\hbar^2G_{min}^2}{2m_e}<\frac{\hbar^2 G^2}{2m_e}<\frac{\hbar^2G_{max}^2}{2m_e}=\mathrm{ENCUTGW}</math>
-This kernel ''squeezes'' contributions from large wave vectors <math>G>G_{max}</math> into the window given by {{TAGBL|ENCUTGWSOFT}}. Effectively, this extrapolates the RPA correlation energy to the {{TAG|ENCUTGW}} <math>\to \infty</math> limit, assuming that the basis set incompleteness error falls off as <math>1/\mathrm{ENCUTGW}^{3/2}</math>.
+This kernel 'squeezes' the contributions from large wave vectors <math>G>G_{max}</math> into the window given by {{TAG|ENCUTGWSOFT}}. Effectively, this extrapolates the random-phase-approximation&ndash;correlation energy to the {{TAG|ENCUTGW}} <math>\to \infty</math> limit, assuming that the basis set incompleteness error falls off as <math>1/</math>{{TAG|ENCUTGW}}<math>^{3/2}</math>.
 == Related Tags and Sections ==
 {{TAG|ENCUTGW}},