URijkl: Difference between revisions

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{{NB|mind|Available as of VASP.6.5.2.}}
This file stores the effectively screened off-centre Coulomb integrals
This file stores the effectively screened off-centre Coulomb integrals
::<math>
::<math>
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     2  1  1  1        0.0324545667      -0.0000455665
     2  1  1  1        0.0324545667      -0.0000455665
   ...
   ...
These integrals are written as a post-processing step using {{TAG|ALGO}}=2e4wa. In contrast to {{FILE|VRijkl}}, the bare off-centre Coulomb integrals, {{FILE|URijkl}} is only written if all {{FILE|WFULLxxxx.tmp}} files commensurate with the selected k-point grid are present in the working directory.
The Coulomb integrals are computed and written as a post-processing step using {{TAG|ALGO}}=2e4wa.  
The basis set can be set with {{TAG|DMFT_BASIS}}.  
The process differs for two types of integrals:
* {{FILE|VRijkl}} (bare off-centre Coulomb integrals): Always written when requested.
* {{FILE|URijkl}}: Only written if all {{FILE|WFULLxxxx.tmp}} files matching the selected k-point grid are present in the working directory.


Evaluation of Coulomb integrals can be computationally demanding if the number of basis functions becomes large.  
The basis set for these calculations can be specified using the {{TAG|DMFT_BASIS}} tag.
{{NB|tip|Use a coarser sub-grid of the original k-point grid with {{TAG|LDOWNSAMPLE}} for speed up.}}
 
{{NB|mind|Available as of VASP.6.5.2.}}
Evaluating Coulomb integrals can be computationally intensive,
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.}}
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[[Category:Files]][[Category:Output files]][[Category:Constrained-random-phase approximation]]
[[Category:Files]][[Category:Output files]][[Category:Constrained-random-phase approximation]]

Revision as of 09:17, 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.