Difference between revisions of "Calculating optical spectra including excitonic effects: a step-by-step guide"

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The target quantity in a Bethe-Salpeter calculation is the macroscopic dielectric matrix &epsilon;<sub>M</sub>. The following quantities/steps are needed to obtain &epsilon;<sub>M</sub>:  
The target quantity in a Bethe-Salpeter calculation is the macroscopic dielectric matrix &epsilon;<sub>M</sub>. The following quantities/steps are needed to obtain &epsilon;<sub>M</sub>:  


[[File:Scheme1.png|500px|center|BSE calculation scheme]]
[[File:Scheme1b.png|500px|center|BSE calculation scheme]]


The optical absorption spectrum corresponds to Im&epsilon;<sub>M</sub>(&omega;). Following this scheme we go through the flow of a calculation:
The optical absorption spectrum corresponds to Im&epsilon;<sub>M</sub>(&omega;). Following this scheme we go through the flow of a calculation:

Revision as of 12:05, 23 March 2021

This tutorial guides you through the workflow of a calculation of the optical spectrum of a given material by solving the Bethe-Salpeter equation. Specifically we will use bulk h-BN as an example.

Atomic structure of bulk hBN

Before starting, you need to obtain the tarballs for hBN. See instructions on the main tutorials page.

The target quantity in a Bethe-Salpeter calculation is the macroscopic dielectric matrix εM. The following quantities/steps are needed to obtain εM:

BSE calculation scheme

The optical absorption spectrum corresponds to ImεM(ω). Following this scheme we go through the flow of a calculation:

Step 1: Static screening

Use the SAVE folders that are already provided and do:

$ cd YAMBO_TUTORIALS/hBN/YAMBO

Follow the Static screening module and then return to this tutorial

Step 2: Bethe-Salpeter kernel

Follow the module on Bethe-Salpeter kernel and return to this tutorial

Step 3: Diagonalisation of the excitonic Hamiltonian

This is the final step in which you finally obtained the spectra. Mathematically this implies to solve a large eigenvalue problem.

Part that should be moved to solvers tutorial

Two main solvers are available in yambo

(1) diagonalization of the full Hamiltonian (diagonalization solver)

(2) subspace iterative | Lanczos algorithm which by-pass diagonalization with the Haydock approach[1] (Lanczos-Haydock solver)

For (1) follow the module on Bethe-Salpeter solver: diagonalization then either return to this tutorial or follow the link to Bethe-Salpeter solver: Lanczos-Haydock for (2).

End part that should be moved to solvers tutorial

Step 4: Include previous quasiparticle (GW) results

Follow the module on Including quasiparticle database and return to this tutorial


References

  1. R. Haydock, in Solid State Phys., 35 215 (1980) edited by H. Ehrenfest, F. Seitz, and D. Turnbull, Academic Press