Abstract
The recent surge of interest in polaritons has prompted fundamental questions about
the role of dark states in strong light-matter coupling phenomena. Here, we systematically
vary the relative number of dark state polaritons by controlling the number of
stacked CdSe nanoplatelets confined in a Fabry-Pérot cavity. We find the emission spectrum
to change significantly with an increasing number of nanoplatelets, with a gradual
shift of the dominant emission intensity from the lower polariton branch to a manifold
of dark states. Through accompanying calculations based on a kinetic model, this shift is rationalized by an entropic trapping of excitations by the dark state manifold, while
a weak dark state dispersion due to local disorder explains their non-zero emission. Our
results point towards the relevance of the dark state concentration to the optical and
dynamical properties of cavity-embedded quantum emitters with ramifications for Bose-
Einstein condensate formation, polariton lasing, polariton-based quantum transduction
schemes, and polariton chemistry.
Supplementary materials
Title
Supplementary Information: Dark State Concentration Dependent Emission and Dynamics of CdSe Nanoplatelet Exciton-Polaritons
Description
The supporting information includes further synthetic details and a characterization of the
CdSe NPLs, the fabrication of the NPL-cavity device, a schematic of the NPL film formation
procedure, scanning tunneling electron microscopy (STEM) images of a single the CdSe
NPL film layer showing their typical face down orientation within the cavity, analysis of the
nanostructral uniformity of the NPLs from STEM images, details and a schematic of the
Fourier spectroscopic set-up used for reflectance and emission measurements, details on the
determination of the cavity linewidth, the angle dependence of the bare exciton reflectance
and emission profiles, angle resolved reflectance measurements for X = 1 through 5, duplicate
reflactance measurements, and comparison of experimental and simulated angle dependent
emission for X = 2 through 4. It also includes the polaritonic Hamiltonian and a derivation
of the phonon mediated exciton-polariton rate equation used in the kinetic model.
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