Single DBT molecules under strong continuous-wave drive show fluorescence suppression and extra line broadening, breaking the two-level saturation model, and an excited-state absorption model reproduces the curves.
Lattice quantum electrodynamics of a molecular emitter in a topological gap
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abstract
Engineering the photonic environment using lattices of coupled resonators, which we refer to as lattice quantum electrodynamics (QED), provides a route to control both the spontaneous emission of individual quantum emitters and the photon-mediated interactions between them. Here we introduce an optical lattice QED platform based on individual dibenzoterrylene (DBT) molecules embedded in anthracene crystals and coupled to lattices of open optical microcavities. This hybrid architecture benefits from narrow-linewidth molecular emitters, site-resolved optical access, engineered coupled-resonator bands, and compatibility with established molecular frequency-tuning techniques. As a proof-of-principle demonstration, we observe emitter-photon bound states formed when the optical transition of a single molecule is tuned to the band gap of a Su-Schrieffer-Heeger (SSH) cavity lattice. These in-gap states display directional localization and photon emission on a single sublattice, inherited from the vacancy-induced topological edge modes of the underlying SSH lattice. Our results establish open-cavity lattices coupled to DBT molecules as a versatile architecture for engineering many-emitter quantum optical systems with controllable photon-mediated interactions.
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Breakdown of the optical saturation regime in molecular single-photon emitters
Single DBT molecules under strong continuous-wave drive show fluorescence suppression and extra line broadening, breaking the two-level saturation model, and an excited-state absorption model reproduces the curves.