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{{TAGDEF|PREC| [real]}}
{{TAGDEF|PREC|Normal {{!}} Single {{!}} SingleN {{!}} Accurate {{!}} Low {{!}} Medium {{!}} High}}
{{DEF|PREC|2|hallo|1|byebye|2|if [[ICHARG]]{{=}}11}}
{{DEF|PREC|Medium|for VASP.4.X|Normal|since VASP.5.X}}


The precision tag
Description: {{TAG|PREC}} specifies the "precision" mode.
 
----
== Intro ==
{{TAG|PREC}} sets default values for the energy cutoff {{TAG|ENCUT}}, the FFT grids ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}) and ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}}), and the accuracy of the projectors in real space {{TAG|ROPT}} (used only when {{TAG|LREAL}}=.TRUE.). Details are given below in the table.
 
An equation
 
<math>
\frac{e}{\pi}=2y
</math>
 
or [[PREC#eqnarray|an equation array]]
 
and set some tags into your {{FILE|INCAR}} file


PREC = A
We recommend using {{TAG|PREC}}=Normal or {{TAG|PREC}}=Accurate. {{TAG|PREC}}=Normal can be used for most routine calculations. {{TAG|PREC}}=Accurate leads to a denser grid ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}). Thus, it reduces egg-box effects and strictly avoids any [[Wrap-around errors|aliasing/wrap-around errors]]. {{TAG|PREC}}=Normal and {{TAG|PREC}}=Accurate use an augmentation fine grid ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}}) that is twice larger than the grid ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}) used for the representation of the pseudo-orbitals. {{TAG|PREC}}=Accurate increases the memory requirements somewhat, but it should be used (in combination with an increased value for {{TAG|ENCUT}}) when a very good accuracy is required, e.g., for accurate forces, for phonons and stress tensor or in general when second derivatives are computed. The accuracy of forces can also be sometimes further improved by specifying {{TAG|ADDGRID}}=.TRUE., however, reports from users are somewhat contradictory about whether this really helps.
GGA  = PE
{{NB|mind|
*The value of a parameter set by {{TAG|PREC}} (e.g., {{TAG|ENCUT}}) can be overridden by specifying explicitly the value of that parameter in the {{FILE|INCAR}} file.
*{{TAG|PREC}}{{=}}Normal and {{TAG|PREC}}{{=}}Accurate are only available in VASP.4.5 and newer versions. The setting {{TAG|PREC}}{{=}}Single is only available as of VASP.5.1, and has been updated in VASP.6.}}
{{NB|deprecated|The old settings {{TAG|PREC}}{{=}}Medium and {{TAG|PREC}}{{=}}High are no longer recommended and are available (as well as {{TAG|PREC}}{{=}}Low) only for backward compatibility. Essentially, {{TAG|PREC}}{{=}}High only increases the energy cutoff by 30 %, which can also be achieved by just manually increasing {{TAG|ENCUT}}.}}
{{NB|important|
*Setting {{TAG|PREC}}{{=}}Accurate does not necessarily mean that the results are converged. The convergence of the results with respect to the energy cutoff {{TAG|ENCUT}} has to be checked separately.
*We strongly recommend specifying the energy cutoff {{TAG|ENCUT}} always manually in the {{FILE|INCAR}} file to ensure the same accuracy between calculations. Otherwise, the default {{TAG|ENCUT}} may differ among the different calculations (e.g., for the calculation of the cohesive energy), with the consequence that the total energies, for instance, can not be compared.
*Setting {{TAG|ENAUG}} has an effect only if {{TAG|PREC}} is set to one of the deprecated settings (Low, Medium or High); otherwise, it is ignored.}}


== And another section ==
== Default values set by {{TAG|PREC}} ==


Default values set by {{TAG|PREC}} for the parameters {{TAG|ENCUT}}, ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}), ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}}) and {{TAG|ROPT}}:


and an array of equations
::{| cellpadding="6" cellspacing="0" border="1"
|{{TAG|PREC}} ||align="center"|{{TAG|ENCUT}} ||align="center"| {{TAG|NGX}},[[NGY|Y]],[[NGZ|Z]] ||align="center"| {{TAG|NGXF}},[[NGYF|YF]],[[NGZF|ZF]] ||align="center"| {{TAG|ROPT}} ({{TAG|LREAL}}=A) ||align="center"| {{TAG|ROPT}} ({{TAG|LREAL}}=O)
|-
| Normal ||align="center"|max({{TAG|ENMAX}}) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"|2&times;{{TAG|NGX}} ||align="center"|-5&times;10<sup>-4</sup> ||align="center"| 1.0
|-
| Single (VASP.5) ||align="center"|max({{TAG|ENMAX}}) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"|{{TAG|NGX}} ||align="center"|-5&times;10<sup>-4</sup> ||align="center"| 1.0
|-
| Single (VASP.6) ||align="center"|max({{TAG|ENMAX}}) ||align="center"| 2&times;<math>G_{\rm cut}</math> ||align="center"|{{TAG|NGX}} ||align="center"|-5&times;10<sup>-4</sup> ||align="center"| 1.0
|-
| SingleN (VASP.6) ||align="center"|max({{TAG|ENMAX}}) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"|{{TAG|NGX}} ||align="center"| -5&times;10<sup>-4</sup> ||align="center"| 1.0
|-
| Accurate ||align="center"|max({{TAG|ENMAX}}) ||align="center"|2&times;<math>G_{\rm cut}</math> ||align="center"|2&times;{{TAG|NGX}}||align="center"|-2.5&times;10<sup>-4</sup> ||align="center"| 1.0
|-
| colspan="6" | '''Deprecated settings:'''
|-
| Low ||align="center"|max({{TAG|ENMIN}}) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"|3&times;<math>G_{\rm aug}</math> ||align="center"|-1&times;10<sup>-2</sup> ||align="center"| 2/3
|-
| Medium ||align="center"|max({{TAG|ENMAX}}) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"|4&times;<math>G_{\rm aug}</math> ||align="center"|-2&times;10<sup>-3</sup> ||align="center"| 1.0
|-
| High || 1.3&times;max({{TAG|ENMAX}}) ||align="center"|2&times;<math>G_{\rm cut}</math> ||align="center"|16/3&times;<math>G_{\rm aug}</math> ||align="center"|-4&times;10<sup>-4</sup> ||align="center"| 1.5
|}
where max({{TAG|ENMAX}}) and max({{TAG|ENMIN}}) are the maxima of {{TAG|ENMAX}} and {{TAG|ENMIN}} found in the {{FILE|POTCAR}} file, and <math>G_{\rm cut}</math> and <math>G_{\rm aug}</math> are defined by
:<math>E_{\rm cut}=\frac{\hbar^2}{2m_e}G_{\rm cut}^2 \qquad E_{\rm aug}=\frac{\hbar^2}{2m_e}G_{\rm aug}^2</math>
with <math>E_{\rm cut}</math>={{TAG|ENCUT}} and <math>E_{\rm aug}</math>={{TAG|ENAUG}}.


<span id="eqnarray">An eqnarray</span>
== Further remarks ==


<math>
*With {{TAG|PREC}}=Normal, Single, and Accurate the grid ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}}) representing the augmentation charges, charge densities and potentials has either the same size ({{TAG|PREC}}=Single) or the double size ({{TAG|PREC}}=Normal or Accurate) as the grid ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}). With the deprecated (and no longer recommended) settings for {{TAG|PREC}} (Low, Medium and High), the grid ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}}) is determined by some heuristic formula from {{TAG|ENAUG}}.
\begin{align}
\frac{e}{\pi} & =\int_\Omega \psi (\mathbf{r}) d\mathbf{r} \\
a & = b \\
\end{align}
</math>


*{{TAG|PREC}}=Single uses the same grid ({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}) as {{TAG|PREC}}=Normal in VASP.5, but the same grid as {{TAG|PREC}}=Accurate in VASP.6. However, the double grid technique is not used, i.e., ({{TAG|NGXF}},{{TAG|NGYF}},{{TAG|NGZF}})=({{TAG|NGX}},{{TAG|NGY}},{{TAG|NGZ}}). This is convenient if one needs to cut down on storage demands or if one wants to reduce the size of the files {{FILE|CHG}} and {{FILE|CHGCAR}}. Furthermore, {{TAG|PREC}}=Single avoids high-frequency oscillations caused by the double-grid technique and the resulting Fourier interpolation. It is often expedient for scanning tunneling simulations or other calculations where high-frequency wiggles of the charge density in the vacuum region are undesirable.


== And one more ==
*{{TAG|PREC}}=Medium and {{TAG|PREC}}=Normal should usually be sufficiently accurate and lead to errors of less than 1 meV/atom.


*{{TAG|PREC}}=High should guarantee that the absolute energies are converged to a few meV and the stress tensor converged within a few kBar.


== And again ==
== Related tags and articles ==
{{TAG|NGX}},
{{TAG|NGY}},
{{TAG|NGZ}},
{{TAG|NGXF}},
{{TAG|NGYF}},
{{TAG|NGZF}},
{{TAG|ENCUT}},
{{TAG|ENAUG}},
{{TAG|ENMIN}},
{{TAG|ENMAX}},
{{TAG|ROPT}},
{{TAG|LREAL}},
{{TAG|ADDGRID}},
{{TAG|PRECFOCK}}


{{sc|PREC|Examples|Examples that use this tag}}
----
----
[[The_VASP_Manual|Contents]]


[[Category:INCAR]]
[[Category:INCAR tag]][[Category:Electronic minimization]][[Category:Memory]]

Latest revision as of 10:00, 31 October 2023

PREC = Normal | Single | SingleN | Accurate | Low | Medium | High 

Default: PREC = Medium for VASP.4.X
= Normal since VASP.5.X

Description: PREC specifies the "precision" mode.


PREC sets default values for the energy cutoff ENCUT, the FFT grids (NGX,NGY,NGZ) and (NGXF,NGYF,NGZF), and the accuracy of the projectors in real space ROPT (used only when LREAL=.TRUE.). Details are given below in the table.

We recommend using PREC=Normal or PREC=Accurate. PREC=Normal can be used for most routine calculations. PREC=Accurate leads to a denser grid (NGX,NGY,NGZ). Thus, it reduces egg-box effects and strictly avoids any aliasing/wrap-around errors. PREC=Normal and PREC=Accurate use an augmentation fine grid (NGXF,NGYF,NGZF) that is twice larger than the grid (NGX,NGY,NGZ) used for the representation of the pseudo-orbitals. PREC=Accurate increases the memory requirements somewhat, but it should be used (in combination with an increased value for ENCUT) when a very good accuracy is required, e.g., for accurate forces, for phonons and stress tensor or in general when second derivatives are computed. The accuracy of forces can also be sometimes further improved by specifying ADDGRID=.TRUE., however, reports from users are somewhat contradictory about whether this really helps.

Mind:
  • The value of a parameter set by PREC (e.g., ENCUT) can be overridden by specifying explicitly the value of that parameter in the INCAR file.
  • PREC=Normal and PREC=Accurate are only available in VASP.4.5 and newer versions. The setting PREC=Single is only available as of VASP.5.1, and has been updated in VASP.6.
Deprecated: The old settings PREC=Medium and PREC=High are no longer recommended and are available (as well as PREC=Low) only for backward compatibility. Essentially, PREC=High only increases the energy cutoff by 30 %, which can also be achieved by just manually increasing ENCUT.
Important:
  • Setting PREC=Accurate does not necessarily mean that the results are converged. The convergence of the results with respect to the energy cutoff ENCUT has to be checked separately.
  • We strongly recommend specifying the energy cutoff ENCUT always manually in the INCAR file to ensure the same accuracy between calculations. Otherwise, the default ENCUT may differ among the different calculations (e.g., for the calculation of the cohesive energy), with the consequence that the total energies, for instance, can not be compared.
  • Setting ENAUG has an effect only if PREC is set to one of the deprecated settings (Low, Medium or High); otherwise, it is ignored.

Default values set by PREC

Default values set by PREC for the parameters ENCUT, (NGX,NGY,NGZ), (NGXF,NGYF,NGZF) and ROPT:

PREC ENCUT NGX,Y,Z NGXF,YF,ZF ROPT (LREAL=A) ROPT (LREAL=O)
Normal max(ENMAX) 3/2× NGX -5×10-4 1.0
Single (VASP.5) max(ENMAX) 3/2× NGX -5×10-4 1.0
Single (VASP.6) max(ENMAX) NGX -5×10-4 1.0
SingleN (VASP.6) max(ENMAX) 3/2× NGX -5×10-4 1.0
Accurate max(ENMAX) NGX -2.5×10-4 1.0
 Deprecated settings:
Low max(ENMIN) 3/2× -1×10-2 2/3
Medium max(ENMAX) 3/2× -2×10-3 1.0
High 1.3×max(ENMAX) 16/3× -4×10-4 1.5

where max(ENMAX) and max(ENMIN) are the maxima of ENMAX and ENMIN found in the POTCAR file, and and are defined by

with =ENCUT and =ENAUG.

Further remarks

  • With PREC=Normal, Single, and Accurate the grid (NGXF,NGYF,NGZF) representing the augmentation charges, charge densities and potentials has either the same size (PREC=Single) or the double size (PREC=Normal or Accurate) as the grid (NGX,NGY,NGZ). With the deprecated (and no longer recommended) settings for PREC (Low, Medium and High), the grid (NGXF,NGYF,NGZF) is determined by some heuristic formula from ENAUG.
  • PREC=Single uses the same grid (NGX,NGY,NGZ) as PREC=Normal in VASP.5, but the same grid as PREC=Accurate in VASP.6. However, the double grid technique is not used, i.e., (NGXF,NGYF,NGZF)=(NGX,NGY,NGZ). This is convenient if one needs to cut down on storage demands or if one wants to reduce the size of the files CHG and CHGCAR. Furthermore, PREC=Single avoids high-frequency oscillations caused by the double-grid technique and the resulting Fourier interpolation. It is often expedient for scanning tunneling simulations or other calculations where high-frequency wiggles of the charge density in the vacuum region are undesirable.
  • PREC=Medium and PREC=Normal should usually be sufficiently accurate and lead to errors of less than 1 meV/atom.
  • PREC=High should guarantee that the absolute energies are converged to a few meV and the stress tensor converged within a few kBar.

Related tags and articles

NGX, NGY, NGZ, NGXF, NGYF, NGZF, ENCUT, ENAUG, ENMIN, ENMAX, ROPT, LREAL, ADDGRID, PRECFOCK

Examples that use this tag