Abstract

A theoretical variation between the two distinct light–matter coupling regimes, namely weak and strong coupling, becomes uniquely feasible in open optical Fabry—Pérot microcavities with low mode volume, as discussed here. In combination with monolayers of transition-metal dichalcogenides (TMDCs) such as WS2, which exhibits a large exciton oscillator strength and binding energy, the room-temperature observation of hybrid bosonic quasiparticles, referred to as exciton–polaritons and characterized by a Rabi splitting, comes into reach. In this context, our simulations using the transfer-matrix method show how to tailor and alter the coupling strength actively by varying the relative field strength at the excitons’ position – exploiting a tunable cavity length, a transparent PMMA spacer layer and angle-dependencies of optical resonances. Continuously tunable coupling for future experiments is hereby proposed, capable of real-time adjustable Rabi splitting as well as switching between the two coupling regimes. Being nearly independent of the chosen material, the suggested structure could also be used in the context of light–matter-coupling experiments with quantum dots, molecules or quantum wells. While the adjustable polariton energy levels could be utilized for polariton-chemistry or optical sensing, cavities that allow working at the exceptional point promise the exploration of topological properties of that point.

Highlights

  • A theoretical variation between the two distinct light–matter coupling regimes, namely weak and strong coupling, becomes uniquely feasible in open optical Fabry—Pérot microcavities with low mode volume, as discussed here

  • Thereby, we show that a transition between the weak and strong coupling regime can be observed

  • The cavity length is determined in a way, that the resonance energy of the empty cavity without 2D material overlaps with the bare exciton mode, which is estimated at a wavelength of 617.2 nm by the imaginary part of the refractive index representing the absorption

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Summary

Theoretical Background

The angle of incidence θ thereby alters the cavity mode’s spectral position as well as the relative field strength but in general the cavity’s linewidth γcav, because modifying θ influences the reflectivity of the DBR mirrors For this setup the change is less than 0.1% within the region of experimentally interesting angles (

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