Microscopic theory for electron-phonon coupling in twisted bilayer graphene

Fuente: arXiv
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Autores principales: Zhu, Ziyan, Devereaux, Thomas P.
Formato: Preprint
Publicado: 2024
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author Zhu, Ziyan
Devereaux, Thomas P.
author_facet Zhu, Ziyan
Devereaux, Thomas P.
contents The origin of superconductivity in twisted bilayer graphene -- whether phonon-driven or electron-driven -- remains unresolved, in part due to the absence of a quantitative and efficient model for electron-phonon coupling (EPC). In this work, we develop a first-principles-based microscopic theory to calculate EPC in twisted bilayer graphene for arbitrary twist angles without requiring a periodic moiré supercell. Our approach combines a momentum-space continuum model for both electronic and phononic structures with a generalized Eliashberg-McMillan theory beyond the adiabatic approximation. Using this framework, we find that the EPC is strongly enhanced near the magic angle. The superconducting transition temperature induced by low-energy phonons peaks at $1.1^\circ$ around 1 K, and remains finite for a range of angles both below and above the magic angles. We predict that superconductivity persists up to $\sim 1.4^\circ$, where superconductivity has been recently observed despite the dispersive electronic bands. Beyond a large density of states, we identify a key condition for strong EPC: resonance between the electronic bandwidth and the dominant phonon frequencies. We also show that the EPC strength of a specific phonon corresponds to the modification of the moiré potential. In particular, we identify several $Γ$-phonon branches that contribute most significantly to the EPC, which are experimentally detectable via Raman spectroscopy.
format Preprint
id arxiv_https___arxiv_org_abs_2407_03293
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Microscopic theory for electron-phonon coupling in twisted bilayer graphene
Zhu, Ziyan
Devereaux, Thomas P.
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
Superconductivity
The origin of superconductivity in twisted bilayer graphene -- whether phonon-driven or electron-driven -- remains unresolved, in part due to the absence of a quantitative and efficient model for electron-phonon coupling (EPC). In this work, we develop a first-principles-based microscopic theory to calculate EPC in twisted bilayer graphene for arbitrary twist angles without requiring a periodic moiré supercell. Our approach combines a momentum-space continuum model for both electronic and phononic structures with a generalized Eliashberg-McMillan theory beyond the adiabatic approximation. Using this framework, we find that the EPC is strongly enhanced near the magic angle. The superconducting transition temperature induced by low-energy phonons peaks at $1.1^\circ$ around 1 K, and remains finite for a range of angles both below and above the magic angles. We predict that superconductivity persists up to $\sim 1.4^\circ$, where superconductivity has been recently observed despite the dispersive electronic bands. Beyond a large density of states, we identify a key condition for strong EPC: resonance between the electronic bandwidth and the dominant phonon frequencies. We also show that the EPC strength of a specific phonon corresponds to the modification of the moiré potential. In particular, we identify several $Γ$-phonon branches that contribute most significantly to the EPC, which are experimentally detectable via Raman spectroscopy.
title Microscopic theory for electron-phonon coupling in twisted bilayer graphene
topic Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
Superconductivity
url https://arxiv.org/abs/2407.03293