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{{Available|6.6.0}}
{{Available|6.6.0}}
This file stores the effectively screened off-centre Coulomb integrals
The {{FILE|URijkl}} file stores the effectively screened off-center Coulomb integrals
::<math>
::<math>
U_{ijkl}^{\sigma\sigma'} =  \int {\rm d}{\bf r}\int {\rm d}{\bf r}'
U_{ijkl}^{\sigma\sigma'} =  \int {\rm d}{\bf r}\int {\rm d}{\bf r}'
Line 6: Line 6:
w_{k}^{*\sigma'}({\bf r}'+{\bf R}) w_{l}^{\sigma'}({\bf r}'+{\bf R})
w_{k}^{*\sigma'}({\bf r}'+{\bf R}) w_{l}^{\sigma'}({\bf r}'+{\bf R})
</math>
</math>
The format is as follows:  
evaluated at zero frequency (<math>\omega=0</math>) for all lattice vectors '''R''' commensurate with the selected k-point grid (see [[Constrained–random-phase–approximation formalism#Off-center interactions|off-center interactions]]). The {{FILE|URijkl}} file contains one block per lattice vector. Each block header gives the lattice vector index and its fractional coordinates. The columns I, J, K, L are the Wannier function indices; RE and IM are the real and imaginary parts. The format is as follows:
# U_ijkl = [ij,R|kl,0]  
  # U_ijkl = [ij,R|kl,0]  
#  I  J  K  L          RE(V_IJKL)          IM(V_IJKL)
  #  I  J  K  L          RE(V_IJKL)          IM(V_IJKL)
# R:    1  0.000000  0.000000  0.000000
  # R:    1  0.000000  0.000000  0.000000
    1  1  1  1        4.3457689208        0.0000000000
    1  1  1  1        4.3457689208        0.0000000000
    2  1  1  1        0.0000021313        0.0000001349
    2  1  1  1        0.0000021313        0.0000001349
...  
  ...  
# R:    2  0.000000  0.000000  1.000000
  # R:    2  0.000000  0.000000  1.000000
    1  1  1  1        1.2535567886        0.0000000000
    1  1  1  1        1.2535567886        0.0000000000
    2  1  1  1        0.0324545667      -0.0000455665
    2  1  1  1        0.0324545667      -0.0000455665
  ...
  ...
The Coulomb integrals are computed and written as a post-processing step using {{TAG|ALGO}}=2e4wa.  
The Coulomb integrals are computed and written as a post-processing step using {{TAG|ALGO|2e4wa}}. The process differs for the two types of integrals:
The process differs for two types of integrals:
* {{FILE|VRijkl}} (bare off-center Coulomb integrals): Always written when requested.
* {{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.
* {{FILE|URijkl}}: Only written if all {{FILE|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 {{TAG|LOCALIZED_BASIS}} tag.
The basis set for these calculations can be specified using {{TAG|LOCALIZED_BASIS}} tag.
 
Evaluating Coulomb integrals can be computationally intensive, especially when dealing with a large number of basis functions.
{{NB|tip|To improve performance, use a coarser sub-grid of the original '''k'''-point grid by enabling {{TAG|LDOWNSAMPLE|T}}.}}
 
== Related tags and articles ==
[[Constrained–random-phase–approximation formalism]]
 
Files: {{FILE|VIJKL}}, {{FILE|UIJKL}}, {{FILE|VRijkl}}
 
Tags: {{TAG|LTWO_CENTER}}, {{TAG|LOCALIZED_BASIS}}, {{TAG|ALGO}}


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.}}
== 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 10:50, 20 March 2026

Mind: Available as of VASP 6.6.0

The URijkl file stores the effectively screened off-center Coulomb integrals

[math]\displaystyle{ U_{ijkl}^{\sigma\sigma'} = \int {\rm d}{\bf r}\int {\rm d}{\bf r}' w_{i}^{*\sigma}({\bf r}) w_{j}^{\sigma}({\bf r}) U({\bf r},{\bf r}',\omega) w_{k}^{*\sigma'}({\bf r}'+{\bf R}) w_{l}^{\sigma'}({\bf r}'+{\bf R}) }[/math]

evaluated at zero frequency ([math]\displaystyle{ \omega=0 }[/math]) for all lattice vectors R commensurate with the selected k-point grid (see off-center interactions). The URijkl file contains one block per lattice vector. Each block header gives the lattice vector index and its fractional coordinates. The columns I, J, K, L are the Wannier function indices; RE and IM are the real and imaginary parts. 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 the two types of integrals:

  • VRijkl (bare off-center 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 LOCALIZED_BASIS tag.

Evaluating Coulomb integrals can be computationally intensive, especially when dealing with a large number of basis functions.

Tip: To improve performance, use a coarser sub-grid of the original k-point grid by enabling LDOWNSAMPLE = T.

Related tags and articles

Constrained–random-phase–approximation formalism

Files: VIJKL, UIJKL, VRijkl

Tags: LTWO_CENTER, LOCALIZED_BASIS, ALGO