LTHOMAS: Difference between revisions
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{{TAGDEF|LTHOMAS|.TRUE. {{!}} .FALSE.|.FALSE.}} | {{TAGDEF|LTHOMAS|.TRUE. {{!}} .FALSE.|.FALSE.}} | ||
Description: {{TAG|LTHOMAS}} selects a decomposition of the exchange functional based on Thomas-Fermi screening. | Description: {{TAG|LTHOMAS}} selects a decomposition of the exchange functional based on Thomas-Fermi exponential screening. | ||
---- | ---- | ||
If {{TAG|LTHOMAS}}=.TRUE. the decomposition of the exchange operator (in a range separated hybrid functional) into a short range and a long range part will be based on Thomas-Fermi screening. | If {{TAG|LTHOMAS}}=.TRUE. the decomposition of the exchange operator (in a [[Hybrid functionals: formalism|range-separated hybrid functional]]) into a short range and a long range part will be based on Thomas-Fermi exponential screening. | ||
The Thomas-Fermi screening length ''k''<sub>TF</sub> is specified by means of the {{TAG|HFSCREEN}} tag. | The Thomas-Fermi screening length ''k''<sub>TF</sub> is specified by means of the {{TAG|HFSCREEN}} tag. | ||
For typical semiconductors, a Thomas-Fermi screening length of about 1.8 Å<sup>-1</sup> yields reasonable band gaps. In principle, however, the Thomas-Fermi screening length depends on the valence electron density | For typical semiconductors, a Thomas-Fermi screening length <math>k_{\rm TF}</math> of about 1.8 Å<sup>-1</sup> yields reasonable band gaps. In principle, however, the Thomas-Fermi screening length depends on the valence-electron density. VASP determines <math>k_{\rm TF}</math> from the number of valence electrons (read from the {{FILE|POTCAR}} file) and the volume (leading to an average density <math>\bar{n}</math>) and writes the corresponding value of <math>k_{\rm TF}=\sqrt{4k_{\rm F}/\pi}</math>, where <math>k_{\rm F}=(3\pi^2\bar{n})^{1/3}</math> to the {{FILE|OUTCAR}} file (note that this value is only printed for information; it is not used during the calculation): | ||
Thomas-Fermi vector in A = 2.00000 | Thomas-Fermi vector in A = 2.00000 | ||
Since | |||
The setting of the sX-LDA functional is shown on the [[list_of_hybrid_functionals|page listing the hybrid functionals]]. | |||
{{NB|mind| | |||
*If {{TAG|LTHOMAS}}{{=}}.TRUE., then {{TAG|LHFCALC}}{{=}}.TRUE. is automatically set. | |||
*If {{TAG|LTHOMAS}}{{=}}.TRUE., then {{TAG|AEXX}}{{=}}1 is automatically set, but {{TAG|AEXX}} can be set to another value.}} | |||
{{NB|important|When {{TAG|AEXX}}{{=}}1 (the default for {{TAG|LTHOMAS}}{{=}}.TRUE.), the correlation <math>E_{\mathrm{c}}^{\mathrm{SL}}</math> is not included. However, it can be included by setting {{TAG|ALDAC}}{{=}}1.0 and {{TAG|AGGAC}}{{=}}1.0.}} | |||
Since VASP counts the semi-core states and ''d''-states as valence electrons, although these states do not contribute to the screening, the values reported by VASP are often not recommended. | |||
== Related tags and articles == | == Related tags and articles == | ||
{{TAG|LHFCALC}}, | {{TAG|LHFCALC}}, | ||
{{TAG|HFSCREEN}}, | {{TAG|HFSCREEN}}, | ||
[[ | {{TAG|AEXX}}, | ||
[[ | {{TAG|LMODELHF}}, | ||
{{TAG|LRHFCALC}}, | |||
[[list_of_hybrid_functionals|List of hybrid functionals]], | |||
[[Hybrid_functionals:_formalism|Hybrid functionals: formalism]] | |||
{{sc|LTHOMAS|Examples|Examples that use this tag}} | {{sc|LTHOMAS|Examples|Examples that use this tag}} | ||
Latest revision as of 21:16, 21 October 2025
LTHOMAS = .TRUE. | .FALSE.
Default: LTHOMAS = .FALSE.
Description: LTHOMAS selects a decomposition of the exchange functional based on Thomas-Fermi exponential screening.
If LTHOMAS=.TRUE. the decomposition of the exchange operator (in a range-separated hybrid functional) into a short range and a long range part will be based on Thomas-Fermi exponential screening. The Thomas-Fermi screening length kTF is specified by means of the HFSCREEN tag.
For typical semiconductors, a Thomas-Fermi screening length [math]\displaystyle{ k_{\rm TF} }[/math] of about 1.8 Å-1 yields reasonable band gaps. In principle, however, the Thomas-Fermi screening length depends on the valence-electron density. VASP determines [math]\displaystyle{ k_{\rm TF} }[/math] from the number of valence electrons (read from the POTCAR file) and the volume (leading to an average density [math]\displaystyle{ \bar{n} }[/math]) and writes the corresponding value of [math]\displaystyle{ k_{\rm TF}=\sqrt{4k_{\rm F}/\pi} }[/math], where [math]\displaystyle{ k_{\rm F}=(3\pi^2\bar{n})^{1/3} }[/math] to the OUTCAR file (note that this value is only printed for information; it is not used during the calculation):
Thomas-Fermi vector in A = 2.00000
The setting of the sX-LDA functional is shown on the page listing the hybrid functionals.
| Mind: |
| Important: When AEXX=1 (the default for LTHOMAS=.TRUE.), the correlation [math]\displaystyle{ E_{\mathrm{c}}^{\mathrm{SL}} }[/math] is not included. However, it can be included by setting ALDAC=1.0 and AGGAC=1.0. |
Since VASP counts the semi-core states and d-states as valence electrons, although these states do not contribute to the screening, the values reported by VASP are often not recommended.
Related tags and articles
LHFCALC, HFSCREEN, AEXX, LMODELHF, LRHFCALC, List of hybrid functionals, Hybrid functionals: formalism