VDW SR: Difference between revisions
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{{TAGDEF|VDW_SR|[real]}} | {{TAGDEF|VDW_SR|[real]}} | ||
Description: {{TAG|VDW_SR}} | Description: {{TAG|VDW_SR}} sets a parameter in the damping function of van der Waals methods. | ||
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{{TAG|VDW_SR}} | {{TAG|VDW_SR}} allows to set the value of a parameter in the following methods: | ||
*Radii scaling <math>s_{r,6}</math> in the dipole-dipole zero-damping function of DFT-D3. {{TAG|VDW_SR}} can be used for both implementations of DFT-D3: [[DFT-D3]] ({{TAG|IVDW}}=11) and [[simple-DFT-D3]] ({{TAG|IVDW}}=15 with {{TAG|SDFTD3_DAMPING}}=zero or mzero). | |||
*Radii scaling <math>s_{R}</math> in the damping function of the Tkatchenko-Scheffler methods ({{TAG|IVDW}}=2 and 21). | |||
*Radii scaling <math>\beta</math> in the damping function of the many-body dispersion energy methods ({{TAG|IVDW}}=202 and 263). | |||
*TT-damping factor <math>b_0</math> in [[DDsC_dispersion_correction|DDsC]] ({{TAG|IVDW}}=4). | |||
== Related tags and articles == | == Related tags and articles == | ||
{{TAG|IVDW}}, | |||
{{TAG|VDW_SR}}, | |||
[[DFT-D3]], | [[DFT-D3]], | ||
[[ | [[simple-DFT-D3]], | ||
[[Tkatchenko-Scheffler_method|Tkatchenko-Scheffler method]], | [[Tkatchenko-Scheffler_method|Tkatchenko-Scheffler method]], | ||
[[Many-body dispersion energy|Many-body dispersion energy]] | [[Tkatchenko-Scheffler method with iterative Hirshfeld partitioning]], | ||
[[Many-body dispersion energy|Many-body dispersion energy]], | |||
[[Many-body dispersion energy with fractionally ionic model for polarizability]], | |||
[[DDsC_dispersion_correction|DDsC]] | |||
{{sc|VDW_SR|Examples|Examples that use this tag}} | {{sc|VDW_SR|Examples|Examples that use this tag}} | ||
Latest revision as of 11:12, 2 March 2026
VDW_SR = [real]
Description: VDW_SR sets a parameter in the damping function of van der Waals methods.
VDW_SR allows to set the value of a parameter in the following methods:
- Radii scaling [math]\displaystyle{ s_{r,6} }[/math] in the dipole-dipole zero-damping function of DFT-D3. VDW_SR can be used for both implementations of DFT-D3: DFT-D3 (IVDW=11) and simple-DFT-D3 (IVDW=15 with SDFTD3_DAMPING=zero or mzero).
- Radii scaling [math]\displaystyle{ s_{R} }[/math] in the damping function of the Tkatchenko-Scheffler methods (IVDW=2 and 21).
- Radii scaling [math]\displaystyle{ \beta }[/math] in the damping function of the many-body dispersion energy methods (IVDW=202 and 263).
- TT-damping factor [math]\displaystyle{ b_0 }[/math] in DDsC (IVDW=4).
Related tags and articles
IVDW, VDW_SR, DFT-D3, simple-DFT-D3, Tkatchenko-Scheffler method, Tkatchenko-Scheffler method with iterative Hirshfeld partitioning, Many-body dispersion energy, Many-body dispersion energy with fractionally ionic model for polarizability, DDsC