URijkl: Difference between revisions
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especially when dealing with a large number of basis functions. | especially when dealing with a large number of basis functions. | ||
{{NB|tip|To improve performance, you can use a coarser sub-grid of the original k-point grid by enabling the {{TAG|LDOWNSAMPLE}} tag.}} | {{NB|tip|To improve performance, you can use a coarser sub-grid of the original k-point grid by enabling the {{TAG|LDOWNSAMPLE}} tag.}} | ||
== Related files == | |||
{{FILE|VIJKL}},{{FILE|UIJKL}},{{FILE|VRijkl}} | |||
---- | ---- | ||
[[Category:Files]][[Category:Output files]][[Category:Constrained-random-phase approximation]] | [[Category:Files]][[Category:Output files]][[Category:Constrained-random-phase approximation]] |
Latest revision as of 09:24, 28 March 2025
Mind: Available as of VASP.6.5.2. |
This file stores the effectively screened off-centre Coulomb integrals
The format is as follows:
# U_ijkl = [ij,R|kl,0] # I J K L RE(V_IJKL) IM(V_IJKL) # R: 1 0.000000 0.000000 0.000000 1 1 1 1 4.3457689208 0.0000000000 2 1 1 1 0.0000021313 0.0000001349 ... # R: 2 0.000000 0.000000 1.000000 1 1 1 1 1.2535567886 0.0000000000 2 1 1 1 0.0324545667 -0.0000455665 ...
The Coulomb integrals are computed and written as a post-processing step using ALGO=2e4wa. The process differs for two types of integrals:
- VRijkl (bare off-centre Coulomb integrals): Always written when requested.
- URijkl: Only written if all WFULLxxxx.tmp files matching the selected k-point grid are present in the working directory.
The basis set for these calculations can be specified using the DMFT_BASIS tag.
Evaluating Coulomb integrals can be computationally intensive, especially when dealing with a large number of basis functions.
Tip: To improve performance, you can use a coarser sub-grid of the original k-point grid by enabling the LDOWNSAMPLE tag. |