Overview

Cavity polaritons in metal lattice plasmon cavities.
Figure 1. Cavity Polaritons in Metal Lattice Plasmon Cavities. Transmission dispersion plots of (a) CdSe NPL film showing absorption by HH and LH excitons, (b) bare Al NP lattice (spacing a0 = 270 nm), (c) CdSe NPL film on Al NP lattice showing band bending with assignments of a lower polariton (LP), middle polariton (MP), and upper polariton (UP). (d) PLdispersion from lower polaritons in strongly coupled system.

Quest. (n) a journey or effort in pursuit of a goal (often lengthy, ambitious, or fervent); a mission.

QuEST. (n) an NSF-funded Phase I Center for Chemical Innovation to discover a new tool that will enable new chemical reactions that are not currently possible; a mission.

QuEST will explore chemical reactions with polaritons, which arise from molecules strongly coupled to an optical cavity.

Objective 1: Better Cavities for Polariton Chemistry

Challenge: to design accessible optical cavities that can facilitate exciton-polariton formation at room temperature

Cavity design considerations

  • Large cavity quality factor (Q)
  • Small mode volume
  • Potential for integration with fluids

QuEST demonstrated strong coupling at 300 K between the heavy and light hole (HH and LH) excitons of CdSe Nanoplatelets (NPLs)(Fig. 1a) and the surface lattice resonances (SLRs) of an aluminum NP lattice (Fig. 1b). The signature of strong coupling is an anti-crossing (or bending) of the energy bands of the cavity photon states when near resonance with the exciton state of the NPL (Fig. 1c). Strong photoluminescence (PL) was also observed coming from the HH lower polariton (Fig. 1d). In an unexpected development, we tailored the position of the lower polariton band and observed ultra-low-threshold polariton lasing from an exciton-polariton condensate (Fig. 2g,h). Our observation of polariton condensation represents a major discovery for a colloidal nanoparticle system in an open architecture nanoparticle lattice cavity.

QuEST is currently exploring the implications of polariton condensates for driving novel chemical reactivity.

Polariton dispersion varies greatly with AI NP lattice cavity properties.
Figure 2. Polariton dispersion varies greatly with Al NP lattice cavity properties. Experimental (top) and simulated (bottom) transmission dispersion diagrams of Al NP lattices coupled to NPL films with lattice periodicities a0 = (a) 270 nm, (b) 310 nm, and (c) 320 nm. (g) Waterfall plot showing emission intensity and wavelength as a function of pump fluence and (inset) real space image of polariton lasing from the lattice. (h) Photoluminescence plot from a0 = 330 lattice showing response at polariton lasing threshold. (j) Polariton lasing peak blue shifts as pump power increases above threshold.

Objective 2: Electrochemical Polariton Characterization

Challenge: determine the absolute energetics of the upper and lower polariton

Polariton Spectroelectrochemical Control.
Figure 3. Polariton Spectroelectrochemical Control. A) Schematic of spectroelectrochemical cell integrated with a metal nanoparticle lattics cavity. B-D) Preliminary results demonstrating the ability to turn strong coupling on and off electrochemically.

QuEST successfully designed and fabricated a prototype spectroelectrochemical cell that employs the optical cavity working electrode and allows optical access with high numerical aperture microscope objectives (Fig. 3). In a major Phase I breakthrough, QuEST was able to successfully manipulate the strength of the coupling between CdSe NPL excitons and the coupled modes of a metal nanoparticle lattice (Fig. 3) by sweeping the applied potential at the working electrode. Such behavior has not been previously seen in a chemically accessible open cavity system. This Phase I accomplishment firmly establishes that exciton-polaritons can reliably and robustly be placed under electrochemical control, and thus provides a clear path to measure absolute polariton energetics, as well as the exciting prospect of ultimately controlling outcomes of chemical reactions through facile tuning of electrochemical potentials.

High Q-Cavity with Upper Polariton PL.
Figure 4. High Q-Cavity with Upper Polariton PL. (left) Reflectance dispersion spectra show strong light-matter coupling with the cavity (top) on resonance and (bottom) blue detuned by 35 meV from the HH exciton for NPLs. (middle) PL dispersion spectra show significant contributions from the UP branch. (right) Quantum dynamics calculations agree with experiemnts and reveal the PL from the UP is a strong function of cavity Q.

Objective 3: Modify Charge Transfer Rates

Challenge: understand how to use an optical cavity to modify the rate of charge transfer between two molecules

Understanding how to control the temporal decay dynamics for polaritons formed between NPLs and dielectric Fabry-Pérot cavities is important because long polariton lifetimes (relative to the cavity radiative lifetime) will establish timescales for chemical reactivity including charge transfers. In an exciting development, we found that increasing the Quality (Q)-factor 6-fold of our Fabry-Pérot optical cavities resulted in photoluminescence emission from the lower (LP) and upper (UP) polariton branches (LP). (Fig. 4) The observation of PL from the UP is a significant milestone as it is exceptionally rare and indeed represents the first time that such upper polariton PL has been observed in a nanoparticle system. Importantly, state-of-the-art theoretical modeling confirmed that the increase in Q-factor was a primary driver of the observation of PL from the UP (Fig. 4).

Polariton PL lifetimes.
Figure 5. Polariton PL lifetimes. (a) PL dispersion used to measure polariton dynamics from CdSe NPLs. (b) Raw PL decay data showing a clear slower decay for uncoupled NPLs relative to NPL polaritons and the instrument response (IRF). (c) Average PL lifetime determined from fits to PL decay curves as a function of cavity detuning.

The increase in cavity Q-factor also enabled a clear measurement of the dynamics from the polariton state. As shown in Fig. 5, we found the PL lifetime for the NPL polariton was around 100 ps (depending on detuning, Fig. 5), in contrast to the lifetime of the bare NPL film outside the cavity, which was 190 ps. The measurement of an unambiguous PL lifetime of the polariton state is a crucial achievement for QuEST in the polariton chemistry field. Importantly, we now have a clear timescale for polariton chemistry events (~ 100 ps), which provides ample time for charge transfers to take place, and allows for facile determination of the effect of strong light-matter coupling on charge transfer rates, which is the subject of ongoing QUEST research in this objective.

Objective 4: Modify Chemical Reactions

Challenge: understand how polaritons alter chemical reactivity and selectivity

An overarching goal of QuEST is to develop strategies to use polaritons to change the selectivity of chemical reactions. While formation of polaritons will alter the electron (density) distribution due to the hybridization of light and matter, it is not known in a general way how polaritons modify molecular orbitals, and how those modified molecular orbitals can lead to new chemical reactivity. Without this understanding, establishing general principles for polariton chemistry will be extremely challenging.

Polariton Modified Reactions.
Figure 6. Polariton Modified Reactions. (a) Ground state polariton energy difference between the meta and ortho-substituted active complex with various field polarizations. Red region corresponds to the ortho-substituted complex and is energetically more stable. (b) Same for para-substituted product. (c) and (d) present the electron density difference analysis between meta-substituted (c) and ortho-substituted (d) intermediates.

Here, we developed an ab-initio theoretical tool to characterize the change of electron density and transition density when coupling molecules to the cavity [24]. Using this new tool, we have explored how cavities can profoundly influence the bromination of nitrobenzene, which in free space yields only a single product: bromination at the meta position (Fig. 6). However, when a nitrobenzene molecule is strongly coupled to the cavity field, the bromination can be tuned by the polarization of cavity electric field to selectively yield either ortho- or para-functionalization. This exciting result stands in direct contradiction with standard chemical intuition and provides a framework for experimental exploration of exciton polariton chemistry.

A large group of people smiling for the camera in a hotel lobby.
QuEST team at the winter conference 2023