Difference between revisions of "Calculating optical spectra including excitonic effects: a step-by-step guide"
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(1) diagonalize the full Hamiltonian (diagonalization solver) | (1) diagonalize the full Hamiltonian (diagonalization solver) | ||
(2) use the subspace iterative [https://en.wikipedia.org/wiki/Lanczos_algorithm| Lanczos algorithm] and by-pass diagonalization with the Haydock approach<ref>R. Haydock, in | (2) use the subspace iterative [https://en.wikipedia.org/wiki/Lanczos_algorithm | Lanczos algorithm] and by-pass diagonalization with the Haydock approach<ref>R. Haydock, in | ||
''Solid State Phys.'', '''35''' 215 (1980) | ''Solid State Phys.'', '''35''' 215 (1980) | ||
edited by H. Ehrenfest, F. Seitz, and D. Turnbull, Academic Press</ref> (Lanczos-Haydock solver) | edited by H. Ehrenfest, F. Seitz, and D. Turnbull, Academic Press</ref> (Lanczos-Haydock solver) |
Revision as of 06:18, 19 April 2017
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.
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:
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. For the CECAM tutorial, 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: Bethe-Salpeter solver
This is the final step in which you finally obtained the spectra. Mathematically this implies to solve a large eigenvalue problem. 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).
References
- ↑ R. Haydock, in Solid State Phys., 35 215 (1980) edited by H. Ehrenfest, F. Seitz, and D. Turnbull, Academic Press