Cavity-field distribution in multiphoton Jaynes-Cummings resonances
arXiv:2201.02092 · doi:10.1103/PhysRevA.104.063717
Abstract
We calculate the cavity-field distribution in the Wigner representation for the two-photon resonance of the weakly driven Jaynes-Cummings (JC) oscillator in its strong-coupling limit. Using an effective four-level system, we analytically demonstrate the presence of steady-state and transient bimodality which breaks azimuthal symmetry in phase space. The two steady-state peaks are located at opposite positions and do not correspond to the two-photon amplitude of the driven transition. The developing bimodality is portrayed in parallel with the evolution of the intensity correlation function for the forwards-scattered photons, before being finally contrasted to the few-photon steady-state and transient phase-space profiles for the cavity mode in the JC model driven on resonance.
8 pages, 4 captioned figures, 27 references, revised Introduction, corrected the exponent in the second line of Eq. (13)
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Cited by in corpus (5)
- Visualizing the breakdown of quantum multimodality in coherently driven light-matter interaction
- Wave-particle correlations in multiphoton resonances of coherent light-matter interaction
- Quantum-fluctuation asymmetry in multiphoton Jaynes-Cummings resonances
- Arbitrary high-fidelity binomial codes from multiphoton spin-boson interactions
- Telling emissions apart in a multiphoton resonance: visualizing a conditional evolution