Local SIC: Difference between revisions

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You can apply the local scaling to PZSIC potentials. The resulting Hamiltonian is as follows,
You can apply the local scaling to PZSIC potentials. The resulting Hamiltonian is as follows,
<math>
<math>
  H_j = - \frac{1}{2} \nabla^2 + v_{ext}(\vec{r})  
  H_j = - \frac{1}{2} \nabla^2 + v_{ext}(\vec{r})  

Revision as of 08:38, 21 August 2022

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PZSIC equation

EPZSIC−DFA=EDFA[ρ↑,ρ↓]−∑i{U[ρiσ]+EXCDFA[ρiσ,0]}.

This is one-electron self-interaction correction scheme and is exact self-interaction cancellation for one electron cases.

LSIC equation

Reference: https://aip.scitation.org/doi/figure/10.1063/1.5129533

In local SIC method, PZSIC energy densities are scaled down with a local scaling factor or iso-orbital indicator z(r).

EXCLSIC−DFA=EXCDFA[ρ↑,ρ↓]−∑i,σocc{ULSIC[ρi,σ]+EXCLSIC[ρi,σ,0]}

where

ULSIC[ρi,σ]=12∫dr→{zσ(r→)}kρi,σ(r→)∫dr′→ρi,σ(r′→)|r→−r′→|

EXCLSIC[ρi,σ,0]=∫dr→{zσ(r→)}kρi,σ(r→)ϵXCDFA([ρi,σ,0],r→).

A typical choice for the local scaling factor is

z(𝐫)=τw(𝐫)τ(𝐫)

This quantity becomes unity at the single orbital regions and becomes zero at the uniform density regions. It cannot differentiate weak interaction regions and uniform density region.

Quasi-SCF approach

You can apply the local scaling to PZSIC potentials. The resulting Hamiltonian is as follows,

Hj=−12∇2+vext(r→)+∫ρ(r′→)|r→−r′→|dr′→+vXCDFA([ρ],r→)−f(r→)(∫ρj(r′→)|r→−r′→|dr′→+vXCDFA([ρj],r→))

Gauge problem

Successes of LSIC method

Static dipole polarizability

water cluster paper

polyacene paper

Mol pol paper

Exchange coupling constant

Reaction barrier height

Anion