Confined Meson Excitations in Rydberg-Atom Arrays Coupled to a Cavity Field
arXiv:2312.17385 · doi:10.1103/PhysRevLett.133.106901
Abstract
Confinement is a pivotal phenomenon in numerous models of high-energy and statistical physics. In this study, we investigate the emergence of confined meson excitations within a one-dimensional system, comprising Rydberg-dressed atoms trapped and coupled to a cavity field. This system can be effectively represented by an Ising-Dicke Hamiltonian model. The observed ground-state phase diagram reveals a first-order transition from a ferromagnetic-subradiant phase to a paramagnetic-superradiant phase. Notably, a quench near the transition point within the ferromagnetic-subradiant phase induces meson oscillations in the spins and leads to the creation of squeezed-vacuum light states. We suggest a method for the photonic characterization of these confined excitations, utilizing homodyne detection and single-site imaging techniques to observe the localized particles. The methodologies and results detailed in this paper are feasible for implementation on existing cavity-QED platforms, employing Rydberg-atom arrays in deep optical lattices or optical tweezers.
13 pages, 8 figures, including supplemental material
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- Digital-Analog Simulations of Schrödinger Cat States in the Dicke-Ising Model
- Meson dynamics from locally exciting a particle-conserving lattice gauge theory
- Amplified response of cavity-coupled quantum-critical systems
- Kinetically constrained cavity QED: from blockaded ferromagnetism to long-range quantum scars