4.6 Article

Quantum phase transition of a two-dimensional Rydberg atom array in an optical cavity

Journal

PHYSICAL REVIEW B
Volume 106, Issue 13, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.106.134506

Keywords

-

Funding

  1. National Science Foundation of China
  2. China Postdoc- toral Science Foundation
  3. Fundamental Research Funds for the Central Universities
  4. [12274046]
  5. [11874094]
  6. [12147102]
  7. [2020M673118]
  8. [2021CDJZYJH- 003]

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The study investigates the behavior of a two-dimensional array of Rydberg atoms in an optical cavity using variational methods and large-scale quantum Monte Carlo simulations. The results show that the strong dipole-dipole interactions between the atoms can lead to a crystal structure, and the coupling between a two-level atom and a cavity photon mode leads to the formation of polaritons. The interplay between these interactions results in a rich quantum phase diagram. This research provides guidance for future experiments.
We study the two-dimensional Rydberg atom array in an optical cavity with the help of a variational method and large-scale quantum Monte Carlo simulations. The strong dipole-dipole interactions between Rydberg atoms can make the system exhibit a crystal structure, and the coupling between a two-level atom and a cavity photon mode can result in the formation of a polariton. The interplay between them provides a rich quantum phase diagram including the Mott, solid-1/2, superradiant, and superradiant solid (SRS) phases. As a two-order coexisted phase, the superradiant solid breaks both translational and U(1) symmetries. Different from the fragile SRS phase in a one-dimensional system [Zhang et al., Phys. Rev. Lett. 110, 090402 (2013)], the SRS phase stays in a larger parameter region. Thus, it is more feasible to detect a SRS phase and corresponding quantum criticality in the real system involving dissipations. Our work not only extends the understanding of the light-atom interacting system, but also provides the guidelines and benchmark for the future experiments.

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