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中国物理学会期刊

磁-腔量子电动力学系统中压缩驱动导致的两体与三体纠缠

CSTR: 32037.14.aps.69.20200838

Bipartite and tripartite entanglement caused by squeezed drive in magnetic-cavity quantum electrodynamics system

CSTR: 32037.14.aps.69.20200838
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  • 本文提出了一种通过压缩驱动放置一个YIG小球的腔量子电动力学(QED)系统产生两体和三体纠缠的理论方案. 微波腔场与铁磁共振(FMR)模和静磁(MS)模的强耦合导致腔内光子、FMR模和MS模之间互相产生纠缠. 稳态情况下, 腔内光子、FMR模和MS模之间可以产生三体纠缠, 其三体纠缠的最小剩余共生纠缠度随非线性增益的增加而增大. 进一步研究发现, 该三体纠缠与MS模式的耗散系数有关, 最小剩余共生纠缠随MS模耗散系数的减小而增大. 同时还发现, 压缩驱动导致的三体纠缠对温度不敏感, 具有很好的鲁棒性. 结果表明磁-腔QED系统是研究宏观量子现象的一个强有力平台.

     

    Utilizing optical nonlinearity for generating the entanglement is still a most widely used approach due to its quality and simplicity. Here in this paper, we propose a theoretical scheme to generate bipartite and tripartite entanglement in a cavity quantum electrodynamics (QED) system with one Yttrium iron garnet (YIG) sphere by using a squeezed drive. In such a system, the parametric down-conversion process is used to generate the nonlinearity and further increase the coupling between cavity and YIG. Thus, the enhanced coupling between the microwave cavity photons and the ferromagnetic resonance (FMR) mode/magnetostatic (MS) mode results in bipartite entanglements. By using the mean field theory, we show that the bipartite entanglements strongly depend on the detuning of the cavity and magnon mode. When the driving field is tuned to be resonant with the FMR mode, but the MS mode is far off-resonant, the entanglement between photons and the FMR mode reaches its maximum. However, when the driving field is tuned to be resonant with the MS mode, but the FMR mode is detuned very well, the entanglement between photons and the MS mode reaches its maximum. We show that the dissipation of the FMR/MS mode affects the entanglement greatly, and the bipartite entanglement decreases as the dissipation rate of the FMR/MS mode increases. Under the steady-state approximation, we also show that the tripartite entanglement can be generated, and the minimum residual contangle increases with the enhancement of the nonlinear gain coefficient. With the nonlinearity induced by the parametric down conversion process, the interaction between the driving field and the magnetic-cavity QED system leads to the tripartite entanglement involving the cavity photons, FMR mode and the MS mode. Likewise, we show that the tripartite entanglement also strongly depends on the dissipation rate of MS mode, and the minimum residual contangle increases as the dissipation rate of the MS mode decreases. We also show that the squeezed field induced tripartite entanglement is insensitive to the temperature and has good robustness. Our results suggest that the magnetic-cavity QED system could provide a promising platform for studying the macroscopic quantum phenomena, and the squeezing field opens a new method of generating the entanglement.

     

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