Dynamical screening and excitonic bound states in biased bilayer graphene
Harley D. Scammell, Oleg P. Sushkov

TL;DR
This paper develops a theoretical framework using the Bethe-Salpeter equation to describe both weak and strong excitonic bound states in biased bilayer graphene, highlighting conditions for strong binding that were previously unachieved experimentally.
Contribution
It introduces a dynamical screening approach with Bethe-Salpeter equations to analyze strong excitonic binding in 2D materials, extending beyond the weak binding regime.
Findings
Strong excitonic binding in biased bilayer graphene is theoretically possible.
Conditions for achieving strong binding include bias, gate configuration, and substrate material.
The approach matches experimental data in the weak binding regime.
Abstract
Excitonic bound states are characterised by a binding energy and a single-particle band gap . This work provides a theoretical description for both strong () and weak () excitonic bound states, with particular application to biased bilayer graphene. Standard description of excitons is based on a wave function that is determined by a Schr\"odinger-like equation with screened attractive potential. The wave function approach is valid only in the weak binding regime . The screening depends on frequency (dynamical screening) and this implies retardation. In the case of strong binding, , a wave function description is not possible due to the retardation. Instead we appeal to the Bethe-Salpeter equation, written in terms of the electron-hole Green's function, to solve the…
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