ESF SPLINES: Difference between revisions
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is evaluated on the k-point grid defined in {{FILE|KPOINTS}} and the correlation energy (as its trace) is stored.{{cite|gelbenegger:thesis2018}} | is evaluated on the k-point grid defined in {{FILE|KPOINTS}} and the correlation energy (as its trace) is stored.{{cite|gelbenegger:thesis2018}} | ||
To obtain the correlation energy on a finer k-point grid, more q-points are added using tri-cubic spline interpolation and the resulting energy is compared to the previous correlation energy. | To obtain the correlation energy on a finer k-point grid, more q-points are added using tri-cubic spline interpolation and the resulting energy is compared to the previous correlation energy. | ||
This procedure is repeated {{TAG| | This procedure is repeated {{TAG|ESF_NINTER}} times until the difference in energy between the interpolation steps is less than {{TAG|ESF_CONV}}. | ||
The default settings of {{TAG| | The default settings of {{TAG|ESF_NINTER}} and {{TAG|ESF_CONV}} typically yield similar k-point convergence compared to the k-p perturbation theory approach, where the limit | ||
<math> | <math> | ||
\lim_{\bf q\to 0} \chi_{{\bf G G}'}({\bf q},i\omega) \cdot {\bf V}_{\bf G G'}({\bf q}) | \lim_{\bf q\to 0} \chi_{{\bf G G}'}({\bf q},i\omega) \cdot {\bf V}_{\bf G G'}({\bf q}) | ||
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== Related tags and articles == | == Related tags and articles == | ||
{{TAG|ESF_CONV}}, | {{TAG|ESF_CONV}}, | ||
{{TAG| | {{TAG|ESF_NINTER}}, | ||
{{TAG|LOPTICS}} | {{TAG|LOPTICS}} | ||
Revision as of 14:40, 10 June 2024
ESF_SPLINES = .FALSE. | .TRUE.
Default: ESF_SPLINES = .FALSE.
Description: ESF_SPLINES selects k-point interpolation in ACFDT(R) calculations using tri-cubic splines.
Interpolates the electronic structure factor in ACFDT/RPA calculations using tri-cubic splines to accelerate k-point convergence of the RPA correlation energy. This feature follows the same idea as in coupled cluster calculations.[1]
To this end, the electronic structure factor in the RPA
is evaluated on the k-point grid defined in KPOINTS and the correlation energy (as its trace) is stored.[2] To obtain the correlation energy on a finer k-point grid, more q-points are added using tri-cubic spline interpolation and the resulting energy is compared to the previous correlation energy. This procedure is repeated ESF_NINTER times until the difference in energy between the interpolation steps is less than ESF_CONV. The default settings of ESF_NINTER and ESF_CONV typically yield similar k-point convergence compared to the k-p perturbation theory approach, where the limit is stored to WAVECAR in a preceding DFT calculation using LOPTICS=T.
Tip: This method works for metals and insulators. |
Warning: Remove WAVEDER before running the job and avoid setting LOPTICS. |