Accelerating GW in 2D systems: Difference between revisions
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where L is the length of the cell in the non-periodic z direction. As the q-grid is 2D, we have <math>q_z = 0.</math> | where L is the length of the cell in the non-periodic z direction. As the q-grid is 2D, we have <math>q_z = 0.</math> | ||
To activate the algorithm it is needed to add the RIM_W in your GW input file: | |||
rim_cut # [R] Coulomb potential | |||
HF_and_locXC # [R] Hartree-Fock | |||
gw0 # [R] GW approximation | |||
ppa # [R][Xp] Plasmon Pole Approximation for the Screened Interaction | |||
dyson # [R] Dyson Equation solver | |||
em1d # [R][X] Dynamically Screened Interaction | |||
RIM_W # Activate the RIM_W algorithm | |||
== Links == | == Links == |
Revision as of 13:30, 1 June 2022
Since Yambo v5.1 it is possible to use an algorithm able to accelerate convergences of GW calculations in two-dimensional systems with respect to the k point sampling.
The method is explained in the paper:
Efficient GW calculations in two-dimensional materials through a stochastic integration of the screened potential
A. Guandalini, P. D'Amico, A. Ferretti and D. Varsano
available at the link: https://arxiv.org/abs/2205.11946
The method makes use of a truncated Coulomb potential in a slab geometry that in Fourier space reads:
[math]\displaystyle{ V_G(q)=\frac{4\pi}{\vert q+G \vert^2}[1-e^{-\vert q_\parallel+G_\parallel\vert L/2}cos[(q_z+G_z)L/2)] }[/math]
where L is the length of the cell in the non-periodic z direction. As the q-grid is 2D, we have [math]\displaystyle{ q_z = 0. }[/math]
To activate the algorithm it is needed to add the RIM_W in your GW input file:
rim_cut # [R] Coulomb potential HF_and_locXC # [R] Hartree-Fock gw0 # [R] GW approximation ppa # [R][Xp] Plasmon Pole Approximation for the Screened Interaction dyson # [R] Dyson Equation solver em1d # [R][X] Dynamically Screened Interaction RIM_W # Activate the RIM_W algorithm