Bulletin of the American Physical Society
2024 APS March Meeting
Monday–Friday, March 4–8, 2024; Minneapolis & Virtual
Session D58: Electrons, Phonons, Electron-Phonon Scattering, and Phononics II
3:00 PM–6:00 PM,
Monday, March 4, 2024
Room: 205D
Sponsoring
Unit:
DCOMP
Chair: Xiao Zhang, University of Michigan
Abstract: D58.00002 : Phonon Self-Energy Corrections: To Screen, or Not to Screen*
3:36 PM–3:48 PM
Presenter:
Samuel Poncé
(European Theoretical Spectroscopy Facility, Institute of Condensed Matter and Nanosciences, Université catholique de Louvain, 1348 Louvain-la-Neuve, Belgium)
Authors:
Jan Berges
(U Bremen Excellence Chair, Bremen Center for Computational Materials Science, and MAPEX Center for Materials and Processes, University of Bremen, 28359 Bremen, Germany)
Nina Girotto
(Institute of Physics, 10000 Zagreb, Croatia)
Tim Wehling
(Institute of Theoretical Physics, University of Hamburg, 22607 Hamburg, Germany)
Nicola Marzari
(Ecole Polytechnique Federale de Lausanne)
Samuel Poncé
(European Theoretical Spectroscopy Facility, Institute of Condensed Matter and Nanosciences, Université catholique de Louvain, 1348 Louvain-la-Neuve, Belgium)
electrons.
The exact phonon self-energy involves a product of a bare and a screened electron-phonon vertex [1] but is inaccessible for practical calculations. In most cases, the exact electron-phonon vertex is approximated by a static mean-field one. Within this approximation, we find that using two screened electron-phonon vertices yields more accurate results than using one bare and one screened vertex due to designed error cancellation to first order [2], but there is no clear path for improvements.
We therefore propose a holistic strategy based on downfolding to partially screened phonons and interactions [3], opening the way to strongly correlated materials and the frequency dependence of the electron-phonon vertex.
[1] F. Giustino, Rev. Mod. Phys. 89, 015003 (2017)
[2] M. Calandra, G. Profeta, and F. Mauri, Phys. Rev. B 82, 165111 (2010)
[3] Y. Nomura and R. Arita, Phys. Rev. B 92, 245108 (2015)
*We acknowledge support from the Deutsche Forschungsgemeinschaft (EXC 2077, FOR 5249, and EXC 2056), the Croatian Science Foundation (UIP-2019-04-6869), NCCR MARVEL from the Swiss National Science Foundation (No. 205602), the Fonds de la Recherche Scientifique de Belgique (FRS-FNRS), and the Walloon Region in the strategic axe FRFS-WEL-T.Computational ressources were provided by the North-German Supercomputing Alliance, the Belgian share of the EuroHPC LUMI supercomputer, the Consortium des Équipements de Calcul Intensif (CÉCI), funded by the FRS-FNRS under Grant No. 2.5020.11, and the PRACE-21 resources MareNostrum at BSC-CNS.
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