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.
Actions



![Author ORCID: We display the ORCID iD icon alongside authors names on our website to acknowledge that the ORCiD has been authenticated when entered by the user. To view the users ORCiD record click the icon. [opens in a new tab]](https://www.cambridge.org/engage/assets/public/coe/logo/orcid.png)