ENCUTGWSOFT: Difference between revisions
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{{NB|important|For vasp.6.3 and later releases {{TAG|ENCUTGWSOFT}} always defaults to {{TAG|ENCUTGW}}<math>\times 0.8</math>.}} | {{NB|important|For vasp.6.3 and later releases {{TAG|ENCUTGWSOFT}} always defaults to {{TAG|ENCUTGW}}<math>\times 0.8</math>.}} | ||
Descprition: The flag {{TAG|ENCUTGWSOFT}} sets the energy cutoff for response function, such that it allows to truncate the Coulomb kernel slowly between the energy | Descprition: The flag {{TAG|ENCUTGWSOFT}} sets the energy cutoff for response function, such that it allows to truncate the Coulomb kernel slowly between the energy | ||
specified by {{TAG|ENCUTGWSOFT}} and {{TAG|ENCUTGW}}. | specified by {{TAG|ENCUTGWSOFT}} and {{TAG|ENCUTGW}} using a cosine window function. | ||
---- | ---- | ||
This usually leads to much smoother energy-volume curves in {{TAG|ACFDT calculations}} and {{TAG|MP2 calculations}}. | This usually leads to much smoother energy-volume curves in {{TAG|ACFDT calculations}} and {{TAG|MP2 calculations}}. | ||
Revision as of 12:43, 23 November 2021
ENCUTGWSOFT = [real]
| Default: ENCUTGWSOFT | = ENCUTGW[math]\displaystyle{ \times 0.8 }[/math] | for ALGO=ACFDT |
| = ENCUTGW[math]\displaystyle{ \times 0.8 }[/math] | as of VASP.6.3 | |
| = ENCUTGW | else |
| Important: For vasp.6.3 and later releases ENCUTGWSOFT always defaults to ENCUTGW[math]\displaystyle{ \times 0.8 }[/math]. |
Descprition: The flag ENCUTGWSOFT sets the energy cutoff for response function, such that it allows to truncate the Coulomb kernel slowly between the energy specified by ENCUTGWSOFT and ENCUTGW using a cosine window function.
This usually leads to much smoother energy-volume curves in ACFDT calculations and MP2 calculations. The modified Coulomb kernel is in this case: [math]\displaystyle{ v_{G} = \frac{4 \pi e^2} {G^2} \frac{1}{2} \left( 1 + \cos \left( \pi \, \frac{ \frac{\hbar^{2} G^2 }{2 m_e} - \mathrm{ ENCUTGWSOFT} }{ \mathrm{ENCUTGW} - \mathrm{ENCUTGWSOFT}} \right) \right) \qquad \mbox{for} \quad \frac{\hbar^2 G^2 }{2 m_e} \gt \mathrm{ENCUTGWSOFT} }[/math]
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 contributions from large wave vectors [math]\displaystyle{ G\gt G_{max} }[/math] into the window given by ENCUTGWSOFT. Effectively, this extrapolates the RPA correlation energy to the ENCUTGW [math]\displaystyle{ \to \infty }[/math] limit, assuming that the basis set incompleteness error falls off as [math]\displaystyle{ 1/\mathrm{ENCUTGW}^{3/2} }[/math].
Related Tags and Sections
PRECFOCK, ENCUT, ENCUTGW, GW calculations, LSCK