Many-body cavity quantum electrodynamics with driven inhomogeneous emitters

Quantum emitters coupled to optical resonators are quintessential systems for exploring fundamental phenomena in cavity quantum electrodynamics (cQED) 1 and are commonly used in quantum devices acting as qubits, memories and transducers 2 . Many previous experimental cQED studies have focused on regimes in which a small number of identical emitters interact with a weak external drive 3 – 6 , such that the system can be described with simple, effective models. However, the dynamics of a disordered, many-body quantum system subject to a strong drive have not been fully explored, despite its importance and potential in quantum applications 7 – 10 . Here we study how a large, inhomogeneously broadened ensemble of solid-state emitters coupled with high cooperativity to a nanophotonic resonator behaves under strong excitation. We discover a sharp, collectively induced transparency (CIT) in the cavity reflection spectrum, resulting from quantum interference and collective response induced by the interplay between driven inhomogeneous emitters and cavity photons. Furthermore, coherent excitation within the CIT window leads to highly nonlinear optical emission, spanning from fast superradiance to slow subradiance 11 . These phenomena in the many-body cQED regime enable new mechanisms for achieving slow light 12 and frequency referencing, pave a way towards solid-state superradiant lasers 13 and inform the development of ensemble-based quantum interconnects 9 , 10 . Under strong excitation, inhomogeneously broadened solid-state emitters coupled with high cooperativity to a cavity demonstrate collectively induced transparency and dissipative many-body dynamics, resulting from cavity–ion coupling.