Resonant Dipole-Dipole Interactions in Electromagnetically Induced Transparency
arXiv:2112.02790 · doi:10.1103/PhysRevA.105.063711
Abstract
Resonant dipole-dipole interaction (RDDI) is ubiquitous in light-matter interacting systems and is responsible for many fascinating properties of collective radiations. Here we theoretically investigate the role of RDDI in electromagnetically induced transparency (EIT). The resonant dipole-dipole interactions manifest in the cooperative spontaneous emission of the probe light transition, which give rise a broadened linewidth and associated collective frequency shift. This cooperative linewidth originates from the nonlocal and long-range RDDI, which can be determined by the atomic density, optical depth, and macroscopic length scales of the atomic ensemble. We present that EIT spectroscopy essentially demonstrates all-order multiple scattering of RDDI. Furthermore, we find that EIT transparency window becomes narrower as the cooperative linewidth increases, which essentially reduces the storage efficiency of slow light as EIT-based quantum memory application.
4 figures
References in corpus (8)
- Cooperative atom-light interaction in a blockaded Rydberg ensemble
- Electromagnetically induced transparency with single atoms in a cavity
- Efficient quantum memory for single photon polarization qubits
- Transmission of near-resonant light through a dense slab of cold atoms
- Phase-imprinted multiphoton subradiant states
- Mean field theory of weakly-interacting Rydberg polaritons in the EIT system based on the nearest-neighbor distribution
- Sensitivity of electromagnetically induced transparency to light-mediated interactions
- Nonlinear absorption in interacting Rydberg electromagnetically-induced-transparency spectra on two-photon resonance