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This study investigates bistability in exciton-photon microcavities operating within the ultrastrong-coupling regime, revealing how counter-rotating processes shift hysteresis windows beyond standard strong-coupling predictions. The research advances fundamental understanding of polariton dynamics and nonlinear optical effects essential for developing next-generation quantum photonic devices and simulators.
Bistability of Exciton-Photon Microcavities in the Ultrastrong-Coupling Regime
arXiv:2607.20688v1 Announce Type: new Abstract: We investigate a coherently driven exciton--photon microcavity with Kerr nonlinearity in the ultrastrong-coupling regime. When the lower and upper polariton branches are well separated in energy, the full Hopfield--Rabi--Kerr model reduces to an effective single-mode description of the lower polariton. We analyze the stability of the lower-polariton steady states. We show that the resulting bistability is qualitatively similar to that in the strong-coupling regime. However, in the ultrastrong-coupling regime counter-rotating processes and the diamagnetic $A^{2}$ term renormalize the polariton spectrum and composition, changing the effective detuning $\tilde{\Delta}_{1}$ and nonlinearity $U_{\mathrm{LP}}$ $g$-dependency beyond the strong-coupling (RWA) picture. As a result, although the semiclassical bistability criterion keeps its standard Kerr--oscillator form, the turning points and hysteresis window are shifted relative to the strong-coupling prediction.
Abstract:We investigate a coherently driven exciton--photon microcavity with Kerr nonlinearity in the ultrastrong-coupling regime. When the lower and upper polariton branches are well separated in energy, the full Hopfield--Rabi--Kerr model reduces to an effective single-mode description of the lower polariton. We analyze the stability of the lower-polariton steady states. We show that the resulting bistability is qualitatively similar to that in the strong-coupling regime. However, in the ultrastrong-coupling regime counter-rotating processes and the diamagnetic $A^{2}$ term renormalize the polariton spectrum and composition, changing the effective detuning $\tilde{\Delta}_{1}$ and nonlinearity $U_{\mathrm{LP}}$ $g$-dependency beyond the strong-coupling (RWA) picture. As a result, although the semiclassical bistability criterion keeps its standard Kerr--oscillator form, the turning points and hysteresis window are shifted relative to the strong-coupling prediction.
Quantum Physics (quant-ph); Atomic and Molecular Clusters (physics.atm-clus)
arXiv:2607.20688 [quant-ph]
(or arXiv:2607.20688v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2607.20688 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
https://doi.org/10.1016/j.chaos.2026.118218 Focus to learn more DOI(s) linking to related resources
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