GW Approximation: a Short Introduction - PowerPoint PPT Presentation

1 / 10
About This Presentation
Title:

GW Approximation: a Short Introduction

Description:

The Kohn-Sham energies have not an interpretation as removal/addition ... Adler-Wiser. expression. and W by its RPA expression: Single Plasmon Pole Model for e ... – PowerPoint PPT presentation

Number of Views:404
Avg rating:3.0/5.0
Slides: 11
Provided by: PAS1
Category:

less

Transcript and Presenter's Notes

Title: GW Approximation: a Short Introduction


1
GW Approximationa Short Introduction
2
Motivationwhy to go from DFT to GW?
  • The Kohn-Sham energies have not an interpretation
    as removal/addition energies (Kopman Theorem does
    not hold).
  • Even though, the KS energies can be considered as
    an approximation to the true Quasiparticle
    energies, but they suffer of some problems (for
    example, the band gap underestimation).
  • Need to correct these inaccuracies -gt calculation
    of the GW corrections.

3
Quasiparticle energies
In the quasiparticle (QP) formalism, the energies
and wavefunctions areobtained by the Dyson
equation
QP equation
which is very similar to the Kohn-Sham equation
KS equation
with Vxc that replaces S, the self-energy (a
non-local and energy dependent operator). We can
calculate the QP (GW) corrections to the DFT KS
eigenvalues by 1st order PT
0-order wavefunctions
0-order
Quasiparticle correction
4
The Self-Energy in the GW approximation
Within the GW approximation,S is given by
GW Self-Energy
Dynamical Screened Interaction
Green Function
5
The Green function G
Furthermore, the Green function G is
approximated by the independent particle G(0)
The basic ingredient of G(0) is the Kohn-Sham
electronic structure
6
W and the RPA approximation
and W by its RPA expression
Dynamical Screened Interaction
Coulomb Interaction
Dielectric Matrix
RPA approximation
Independent Particle Polarizability
Adler-Wiser expression
ingredients KS wavefunctions and KS energies
7
Single Plasmon Pole Model for e
The dynamic (w) dependence of the Dielectric
Matrix is modeled with a Plasmon Pole model
Plasmon Pole Model
this gives Sx
this gives Sc
To calculate the 2 parameters of the model, we
need to calculate e in 2 frequencies.
8
Sx (exchange) and Sc (correlation)
Defining r (calculated through FFT)
We arrive at
w-independent, only occupied states
9
Dynamic dependence
S depends on wenk
in principle the non-linear equation should be
solved self-consistently. but we linearize
and defining the renormalization constant Znk
(the derivative is calculated numerically)
renormalization constant
we finally arrive at
10
GW scheme of the calculation
Write a Comment
User Comments (0)
About PowerShow.com