VIJKL: Difference between revisions

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This file stores the bare Coulomb integrals
The {{FILE|VIJKL}} file stores the bare Coulomb integrals at the unit-cell origin ('''R''' = 0):
::<math>
::<math>
V_{ijkl}^{\sigma\sigma'} =  \int {\rm d}{\bf r}\int {\rm d}{\bf r}'
V_{ijkl}^{\sigma\sigma'} =  \int {\rm d}{\bf r}\int {\rm d}{\bf r}'
\frac{ w_{i}^{*\sigma}({\bf r}) w_{j}^{\sigma}({\bf r}) w_{k}^{*\sigma'}({\bf r}') w_{l}^{\sigma'}({\bf r}')}{|{\bf r}-{\bf r}'|}
\frac{ w_{i}^{*\sigma}({\bf r}) w_{j}^{\sigma}({\bf r}) w_{k}^{*\sigma'}({\bf r}') w_{l}^{\sigma'}({\bf r}')}{|{\bf r}-{\bf r}'|}
</math>
</math>
The format is as follows:  
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:
# V_ijkl = [ij,R|kl,0]  
  # V_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)
    1  1  1  1      14.4576272582        0.0000000000
    1  1  1  1      14.4576272582        0.0000000000
    2  1  1  1        0.0000010313        0.0000031049
    2  1  1  1        0.0000010313        0.0000031049
  ...
  ...
== Related files ==
 
{{FILE|UIJKL}},{{FILE|URijkl}},{{FILE|VRijkl}}
== Related tags and articles ==
----
[[Constrained–random-phase–approximation formalism]]
 
Files: {{FILE|UIJKL}}, {{FILE|URijkl}}, {{FILE|VRijkl}}
 
Tags: {{TAG|LOCALIZED_BASIS}}, {{TAG|ALGO}}
 
[[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

The VIJKL file stores the bare Coulomb integrals at the unit-cell origin (R = 0):

[math]\displaystyle{ V_{ijkl}^{\sigma\sigma'} = \int {\rm d}{\bf r}\int {\rm d}{\bf r}' \frac{ w_{i}^{*\sigma}({\bf r}) w_{j}^{\sigma}({\bf r}) w_{k}^{*\sigma'}({\bf r}') w_{l}^{\sigma'}({\bf r}')}{|{\bf r}-{\bf r}'|} }[/math]

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:

 # V_ijkl = [ij,R|kl,0] 
 #  I   J   K   L          RE(V_IJKL)          IM(V_IJKL)
    1   1   1   1       14.4576272582        0.0000000000
    2   1   1   1        0.0000010313        0.0000031049
  ...

Related tags and articles

Constrained–random-phase–approximation formalism

Files: UIJKL, URijkl, VRijkl

Tags: LOCALIZED_BASIS, ALGO