ESF SPLINES: Difference between revisions
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Description: {{TAG|ESF_SPLINES}} selects k-point interpolation in ACFDT(R) calculations using tri-cubic splines. | Description: {{TAG|ESF_SPLINES}} selects k-point interpolation in ACFDT(R) calculations using tri-cubic splines. | ||
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Interpolates the electronic structure factor in [[ACFDT/RPA calculations]] using tri-cubic splines to accelerate k-point convergence of the [[ACFDT:_Correlation_energy_in_the_Random_Phase_Approximation|RPA correlation energy]]. This feature follows the same idea as in coupled cluster calculations.{{cite|liao:jcp:2016}} | Interpolates the electronic structure factor in [[ACFDT/RPA calculations]] using tri-cubic splines to accelerate k-point convergence of the [[RPA/ACFDT:_Correlation_energy_in_the_Random_Phase_Approximation|RPA correlation energy]]. This feature follows the same idea as in coupled cluster calculations.{{cite|liao:jcp:2016}} | ||
To this end, the electronic structure factor in the RPA | To this end, the electronic structure factor in the RPA |
Revision as of 14:32, 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_NITER times until the difference in energy between the interpolation steps is less than ESF_CONV. The default settings of ESF_NITER 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. |