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Bulletin of the American Physical Society

In-plane electrical transport across cavity-quantum well system in Bose-Einstein condensate phase

Ming Xie, Allan H. MacDonald

Published Mar 17, 2016• 0 citations
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The coupled dynamics of the atom and photon fields in optical ring cavities with two counterpropagating modes give rise to both spin-orbit interactions as well as long-ranged interactions between atoms of a many-body system. At zero temperature, the interplay between the two-body and cavity-mediated interactions determines the ground state of a Bose-Einstein condensate. In this work, we find that cavity quantum electrodynamics in the weak-coupling regime favors a stripe-phase state over a plane-wave phase as the strength of cavity-mediated interactions increases. Indeed, the stripe phase is energetically stabilized even for condensates with attractive intraspecies and interspecies interactions for sufficiently large cavity interactions. The elementary excitation spectra in both phases correspond to linear dispersion relation at long wavelengths, indicating that both phases exhibit superfluidity, although the plane-wave phase also displays a characteristic roton-type feature. The results suggest that even in the weak-coupling regime, cavities can yield interesting new physics in ultracold quantum gases.

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Abstract Spin–orbit–coupled Bose–Einstein condensates are a central platform for exploring quantum phase transitions and synthetic quantum matter, yet how entanglement behaves across these transitions remains largely unexplored. We analyze bipartite entanglement between synthetically dressed pseudo–spin states in a cavity–QED environment using a quantum–Langevin approach, where the coupled atom–photon fluctuations are governed by a non-Hermitian drift matrix. Steady-state quantum correlations are quantified through logarithmic negativity and entanglement fidelity. When cavity loss dominates over atomic dissipation, the cavity mediates only dispersive coupling between the pseudo-spins, and the entanglement remains weak and broadly distributed across the transition from the stripe-like mixed state to the plane-wave state. When atomic dissipation becomes the dominant channel, the fluctuation spectrum undergoes a qualitative and topological change: a set of spin-localized, edge-like photonic modes emerges. These non-Hermitian topological edge modes act as spectrally selective pathways that confine cavity-generated fluctuations around the pseudo–spin manifold, enhance their phase-space overlap, and produce sharply bounded regions of strong spin–spin entanglement in the Raman parameter plane. Entanglement fidelity verifies that the enhancement originates from topological edge-mode localization rather than from dissipation itself. Thus, non-Hermitian topological edge physics reorganizes the entanglement landscape across the phase transition of synthetically dressed atomic states, revealing a pathway to edge-mode-enhanced quantum entanglement in hybrid quantum systems.

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Hrishikesh Kelkar, Braulio Gutiérrez–Medina, Kevin C. Henderson +1 more

Bulletin of the American Physical Society•May 19, 2005•0 citations
The coupled dynamics of the atom and photon fields in optical ring cavities with two counterpropagating modes give rise to both spin-orbit interactions as well as long-ranged interactions between atoms of a many-body system. At zero temperature, the interplay between the two-body and cavity-mediated interactions determines the ground state of a Bose-Einstein condensate. In this work, we find that cavity quantum electrodynamics in the weak-coupling regime favors a stripe-phase state over a plane-wave phase as the strength of cavity-mediated interactions increases. Indeed, the stripe phase is energetically stabilized even for condensates with attractive intraspecies and interspecies interactions for sufficiently large cavity interactions. The elementary excitation spectra in both phases correspond to linear dispersion relation at long wavelengths, indicating that both phases exhibit superfluidity, although the plane-wave phase also displays a characteristic roton-type feature. The results suggest that even in the weak-coupling regime, cavities can yield interesting new physics in ultracold quantum gases.
Abstract Spin–orbit–coupled Bose–Einstein condensates are a central platform for exploring quantum phase transitions and synthetic quantum matter, yet how entanglement behaves across these transitions remains largely unexplored. We analyze bipartite entanglement between synthetically dressed pseudo–spin states in a cavity–QED environment using a quantum–Langevin approach, where the coupled atom–photon fluctuations are governed by a non-Hermitian drift matrix. Steady-state quantum correlations are quantified through logarithmic negativity and entanglement fidelity. When cavity loss dominates over atomic dissipation, the cavity mediates only dispersive coupling between the pseudo-spins, and the entanglement remains weak and broadly distributed across the transition from the stripe-like mixed state to the plane-wave state. When atomic dissipation becomes the dominant channel, the fluctuation spectrum undergoes a qualitative and topological change: a set of spin-localized, edge-like photonic modes emerges. These non-Hermitian topological edge modes act as spectrally selective pathways that confine cavity-generated fluctuations around the pseudo–spin manifold, enhance their phase-space overlap, and produce sharply bounded regions of strong spin–spin entanglement in the Raman parameter plane. Entanglement fidelity verifies that the enhancement originates from topological edge-mode localization rather than from dissipation itself. Thus, non-Hermitian topological edge physics reorganizes the entanglement landscape across the phase transition of synthetically dressed atomic states, revealing a pathway to edge-mode-enhanced quantum entanglement in hybrid quantum systems.