BSEPREC: Difference between revisions

Latest revision as of 11:59, 20 October 2023

BSEPREC = Low | Medium | High | Accurate
Default: BSEPREC = Medium

Description: BSEPREC determines the precision of the time-evolution algorithm for solving the Bethe-Salpeter or Casida equations, i.e., the timestep and the number of steps.

The timestep in the time-evolution calculation is inversely proportional to the maximum transition energy OMEGAMAX and the number of steps is inversely proportional to the broadening CSHIFT. Depending on the BSEPREC stable these parameters are scaled depending on the precision tag BSEPREC.

BSEPREC	OMEGAMAX	CSHIFT
Accurate (a)	$\times 4$	$\times 1/10$
High (h)	$\times 3$	$\times 1/7.5$
Medium (m)	$\times 2.5$	$\times1/6.25$
Low (l)	$\times 2$	$\times1/5$

For example, the number of steps $N_{\rm steps}$ for BSEPREC = Low can be found via $N_{\rm steps}=\frac{{\rm OMEGAMAX}\times 2}{{\rm CSHIFT}/5}$

@@ Line 1: / Line 1: @@
 {{TAGDEF|BSEPREC|Low {{!}} Medium {{!}} High {{!}}  Accurate | Medium}}
+Description: {{TAG|BSEPREC}} determines the precision of the time-evolution algorithm for solving the Bethe-Salpeter or Casida equations, i.e., the timestep and the number of steps.
-Description: {{TAG|BSEPREC}} determines the precision for the time-evolution calculation in BSE and TDDFT, i.e., the step size and the number of steps.
 ----
-The timestep size in the time-evolution calculation is inversely proportional to the  maximum transition energy {{TAG|OMEGAMAX}} and the number of steps is inversely proportional to the broadening {{TAG|CSHIFT}}. {{TAG|BSEPREC}} defines
+The timestep in the time-evolution calculation is inversely proportional to the maximum transition energy {{TAG|OMEGAMAX}} and the number of steps is inversely proportional to the broadening {{TAG|CSHIFT}}. Depending on the {{TAG|BSEPREC}}  stable these parameters are scaled depending on the precision tag {{TAG|BSEPREC}}.
-::{| cellpadding="5" cellspacing="0" border="1"
+{| cellpadding="5" cellspacing="0" border="1"
 ! BSEPREC !! OMEGAMAX !! CSHIFT
 |-
-| Accurate (a) || &times;4 || &times;10
+| Accurate (a) || <math>\times 4</math> || <math>\times 1/10</math>
 |-
-| High (h) || &times;3 || &times;7.5
+| High (h) || <math>\times 3</math> || <math>\times 1/7.5</math>
 |-
-| Medium (m) || &times;2.5 || &times;6.25
+| Medium (m) || <math>\times 2.5</math> || <math>\times1/6.25</math>
 |-
-| Low (l)  || &times;2 || &times;5
+| Low (l)  || <math>\times 2</math> || <math>\times1/5</math>
 |}
+For example, the number of steps <math>N_{\rm steps}</math> for {{TAG|BSEPREC}} = Low can be found via <math>N_{\rm steps}=\frac{{\rm OMEGAMAX}\times 2}{{\rm CSHIFT}/5}</math>
 == Related tag and articles ==
+{{TAG|IBSE}},
+{{TAG|NBANDSV}},
 {{TAG|NBANDSO}},
+{{TAG|CSHIFT}},
+{{TAG|OMEGAMAX}},
 [[BSE calculations]],
-[[timepropagation]]
+[[Time-dependent density-functional theory calculations]],
+[[Bethe-Salpeter equations]]
-{{sc|NBANDSV|Examples|Examples that use this tag}}
 ----
 [[Category:INCAR tag]] [[Category:Many-body perturbation theory]][[Category:Bethe-Salpeter equations]]