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In quantum physics, with high principal value can exhibit strong . However, (quasiparticles) with an excitonic constituent in an excited state, known as Rydberg exciton polaritons (REPs) remain to be experimentally observed. In a recent study now published on the Proceedings of the National Academy of Sciences of the United States of America (PNAS). Wei Bao and an interdisciplinary research team in the departments of physics, electronics and the National Science Foundation (NSF) Nanoscale Science and Engineering Center in the U.S., observed the formation of REPs in a (cesium lead bromide) perovskite cavity; without any external fields. The researchers noted the polaritons to exhibit strong nonlinear behavior, which lead to a coherent polariton condensate with a prominent blue shift. The REPs in CsPbBr₃ cavity were highly anisotropic (showing different properties in different directions) with a large due to the orthorhombic crystal structure of the perovskite.

Quantum coherence is only possible in the presence of strong interactions between exciton polaritons due to their excitonic constituents. The observations by Bao et al. shed light on the importance of in coherent polariton systems involving higher-order excited states and paves the way to explore additional coherent interactions. Further investigations will benefit solid-state quantum information processing technologies.

Solid-state cavity quantum electrodynamics (CQED) can deliver extraordinary control of light matter interactions within a . Aside from simply modifying the photonic density of states in the weak coupling regime, CQED can also facilitate the formation of new, hybrid known as . Cavity polaritons are created in semiconductor microcavities (MC) due to strong coupling between excitons and photons, where the coupling rate can be faster than the dissipation rates of the constituents. The possessed a small effective mass from their photonic component to inherit strong interactions from their excitonic component. This combination allowed rich quantum optical phenomena such as polariton condensation, superfluidity and quantum vortices—similar to those observed in (BEC), although at higher temperatures.

Emerging lead halide perovskites with are excellent candidates to investigate exciton-polariton states and polariton condensation for . Â鶹ÒùÔºicists had polariton lasing based on the ground exciton state in a CsPbCl₃ microcavity. In the present work, Bao et al. showed the formation of hybrid exciton polaritons in a single crystal perovskite CsPbCl_3, including emerging REPs without external fields. Importantly, they reached the (an exotic quantum phenomenon observed in dilute atomic gases) of polaritons with a prominent blue shift. The polaritons were anisotropic and the observed, precise polarization control was a necessary prerequisite in quantum optical information processing. The work builds a major step forward in solid-state quantum photonic systems and offers a unique platform for . In parallel, the research also opens a new door to solid-state quantum photonic applications in communication and computing of .

The research team selected the metal halide perovskite (CsPbCl₃) as the exciton host due to its superior chemical stability and emission efficiency compared to . To investigate the strong light-matter interactions in these excitonic states they embedded the CsPbCl₃ microplate in a Fabry-Perot planar cavity (fundamental building block of laser interferometers). This high cavity quality assisted the formation of a REP due to the sharp interface between the perovskite and the metal mirror in the setup, alongside reduced metal absorption losses at .

Bao et al. observed the coherent coupling of these states and cavity photons using k-space spectroscopy after cooling the samples to 90 K. They conducted the k-space characterization using selective linear polarization for photoluminescence (PL) and reflectivity measurements. They measured the PL with a non-resonant pump laser of 460 nm and completed the reflectivity measurements using a non-polarized tungsten halogen white light source. The team obtained two dispersive modes from both PL and reflectivity measurements, which they identified as the newly formed polariton states. The observation implied coherent strong coupling between light and an exciton excited state, without an external field to form the expected REP (Rydberg exciton polariton). The polaritons showed extremely strong polarization anisotropy originating from the perovskite refractive indices.

The researchers defined a (carefully engineered coupling between light and matter) as a coherent ensemble of a finite density of particles in the lowest available polariton state. They described the state using a dissipative . A condensate was possible at higher than cryogenic temperatures due to their small effective mass (approximating 10⁴ electron mass) of the hybrid light-matter particles and the strong interactions among them. At higher carrier densities the interactions became significant to generate a stimulated nonlinear regime to form a macroscopically coherent quantum condensation state.

The scientists performed further analysis to confirm polariton condensation. They observed three corresponding regions; where (1) polariton interactions were insignificant, (2) formed stimulated interactions between REPs, and (3) formed the condensate regime. The results justified the interpretation Bao et al. formed on the non-equilibrium steady state as an exciton-polariton condensate. In contrast to , the research team observed the involvement of multiple polariton modes due to strong exciton-exciton interactions in the study.

The strong interaction of REPs in the nonlinear region was also evident in the blue shifts of these polariton energies; the shift did not occur due to a heating effect at higher laser pump powers. When the researchers extracted the photoluminescence peak positions as a function of pump power, they observed polariton modes below the threshold to show noticeable blue shifts due to small disorder effect. Above the threshold, the repulsive polariton-polariton interactions became more prominent, causing the REP modes to show strong blue shifts. The study demonstrated very strong polariton interactions with the participation of Rydberg excitonic states.

It is beyond the scope of the present work to establish a more detailed theory to accurately calibrate polariton density, alongside quantitative analysis of dipole-dipole interactions and inter-exciton interactions to gain a better estimate of interaction strength. Nevertheless, the present experimental observations of REP with enhanced interactions promise further exploration of Rydberg interactions in solid-state systems in the future.

In this way, Wei Bao and colleagues surprisingly discovered REPs in a single crystal perovskite cavity, providing them coherent control of the observed fine quantum states. The intrinsic strong exciton interaction and optical birefringence in perovskite lead to the observation of polariton-condensation dynamics. This outcome promised a robust macroscopically coherent state for quantum applications. The discovery presents a unique platform to study quantum coherent many-body physics to allow the unprecedented manipulation of these Rydberg states within quantum applications. Bao et al. aim to explore the new states via chemical composition engineering, structural phase control and external gauge fields. The scientists showed that controlling the REP and its condensates added new flavors to study polariton lasing, superfluidity and vortices. Importantly, the work holds great potential to applications in quantum communication and quantum stimulation.

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