NBSEBLOCKO: Difference between revisions

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Description: {{TAG|NBSEBLOCKO}} specifies the blocking factor for the occupied states when setting up the BSE Hamiltonian.
Description: {{TAG|NBSEBLOCKO}} specifies the blocking factor for the occupied states when setting up the BSE Hamiltonian.
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By default, the construction of the BSE Hamiltonian in VASP is parallelized over k-points, such that each MPI rank can compute a pair of k-points. This way the BSE Hamiltonian setup can be parallelized up to <math>\mathrm{NKPTS*(NKPTS+1)/2}</math> MPI ranks or <math>\mathrm{NKPTS*2*(NKPTS*2+1)/2}</math> for spin-polarized case, where <math>\mathrm{NKPTS}</math> is the total number of k-points in the full Brillouin zone. However, if a large number of MPI ranks is used in a calculation with too few k-point, this leads to load imbalance, where some of the MPI rank will have no data to compute. In such cases, it is recommended to use parallelization over bands. If the paralliziation over bands is used, all occupied (unoccupied) bands are divided into a <math>\mathrm{NBLKO (NBLKV)}</math> number of blocks, where <math>\mathrm{NBLKO=NBANDSO/NBSEBLOCKO}</math> and <math>\mathrm{NBLKV=NBANDSV/NBSEBLOCKV}</math>. This bands blocking allows VASP to parallelize the setup of the matrix up to <math>\mathrm{NBLKO*NBLKV*NKPTS*(NBLKO*NBLKV*NKPTS+1)/2}</math> ranks.
By default, the construction of the BSE Hamiltonian in VASP is parallelized over '''k'''-points, such that each MPI rank can compute a pair of '''k'''-points. This way the BSE Hamiltonian setup can be parallelized with
::<math>\text{total ranks}=\mathrm{NKPTS\times(NKPTS+1)/2}</math>  
or for spin-polarized case
::<math>\text{total ranks}=\mathrm{NKPTS\times 2\times(NKPTS\times 2+1)/2}</math>,


If no <math>\mathrm{NBSEBLOCKV}</math> or <math>\mathrm{NBSEBLOCKO}</math> is specified, no paralliziation over bands is used and <math>\mathrm{NBLKO=1 (NBLKV=1)}</math>.
where <math>\mathrm{NKPTS}</math> is the total number of '''k'''-points in the full Brillouin zone. However, if a large number of MPI ranks is used in a calculation with too few '''k'''-point, this leads to load imbalance, where some of the MPI ranks will have no data to compute. In such cases, it is recommended to use parallelization over bands. If the parallelization over bands is used, all occupied (unoccupied) bands are divided into
{{NB|mind|Parallelization over bands with {{TAG|NBSEBLOCKO}} does not work with the old BSE driver, i.e., {{TAG|IBSE}}{{=}}0}}
::<math>\mathrm{NBLKO=NBANDSO/NBSEBLOCKO}</math>  
and  
::<math>\mathrm{NBLKV=NBANDSV/NBSEBLOCKV}</math>
blocks, respectively.


Such a band blocking allows VASP to parallelize the setup of the matrix with
::<math>\text{total ranks}=\mathrm{NBLKO\times NBLKV\times NKPTS\times (NBLKO\times NBLKV\times NKPTS+1)/2}</math>
or for spin-polarized case
::<math>\text{total ranks}=\mathrm{NBLKO\times NBLKV\times NKPTS\times 2\times (NBLKO\times NBLKV\times NKPTS\times 2+1)/2}</math>
If neither <math>\mathrm{NBSEBLOCKV}</math> nor <math>\mathrm{NBSEBLOCKO}</math> is specified, no paralliziation over bands is used and <math>\mathrm{NBLKO=1}</math> and <math>\mathrm{NBLKV=1}</math>.
{{NB|mind|Parallelization over bands with {{TAG|NBSEBLOCKV}} does not work with the old BSE driver, i.e., {{TAG|IBSE}}{{=}}0}}
We recommend using parallelization over bands only if the number of MPI ranks in the calculation exceeds <math>\text{total ranks}</math>.
{{NB|mind|The {{TAG|NBSEBLOCKV}} and {{TAG|NBSEBLOCKO}} tags are available as of VASP.6.5.0}}
== Related tags and sections ==
== Related tags and sections ==
{{TAG|BSE}}, {{TAG|NBSEBLOCKV}}, [[BSE calculations]]
{{TAG|BSE}}, {{TAG|NBSEBLOCKV}}, [[BSE calculations]], [[TDDFT calculations]]


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[[Category:INCAR tag]][[Category:Bethe-Salpeter_equations]][[Category:Many-body perturbation theory]][[Category:GW]]
[[Category:INCAR tag]][[Category:Bethe-Salpeter_equations]][[Category:Many-body perturbation theory]]

Latest revision as of 09:53, 18 December 2024

NBSEBLOCKO = [integer] 

Default: NBSEBLOCKO = -1

Description: NBSEBLOCKO specifies the blocking factor for the occupied states when setting up the BSE Hamiltonian.


By default, the construction of the BSE Hamiltonian in VASP is parallelized over k-points, such that each MPI rank can compute a pair of k-points. This way the BSE Hamiltonian setup can be parallelized with

or for spin-polarized case

,

where is the total number of k-points in the full Brillouin zone. However, if a large number of MPI ranks is used in a calculation with too few k-point, this leads to load imbalance, where some of the MPI ranks will have no data to compute. In such cases, it is recommended to use parallelization over bands. If the parallelization over bands is used, all occupied (unoccupied) bands are divided into

and

blocks, respectively.

Such a band blocking allows VASP to parallelize the setup of the matrix with

or for spin-polarized case

If neither nor is specified, no paralliziation over bands is used and and .

Mind: Parallelization over bands with NBSEBLOCKV does not work with the old BSE driver, i.e., IBSE=0

We recommend using parallelization over bands only if the number of MPI ranks in the calculation exceeds .

Mind: The NBSEBLOCKV and NBSEBLOCKO tags are available as of VASP.6.5.0

Related tags and sections

BSE, NBSEBLOCKV, BSE calculations, TDDFT calculations