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Ultrastrong-coupling regime of nondipolar light-matter interactions

机译:非极硅偏光物相互作用的超空耦合制度

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摘要

We present a circuit-QED scheme which makes it possible to reach the ultrastrong-coupling regime of a nondipolar interaction between a single qubit and a quantum resonator. We show that the system Hamiltonian is well approximated by a two-photon quantum Rabi model and propose a simple scattering experiment to probe its fundamental properties. In particular, we identify a driving scheme that reveals the change in selection rules characterizing the breakdown of the rotating-wave approximation and the transition from strong to ultrastrong two-photon interactions. Finally, we show that a frequency crowding in a narrow spectral region is observable in the output fluorescence spectrum as the coupling strength approaches the collapse point, paving the way to the direct observation of the onset of the spectral collapse in a solid-state device.
机译:我们介绍了一种电路QED方案,其使得可以在单个Qubit和量子谐振器之间达到非极性相互作用的超空耦合状态。 我们表明,系统哈密顿人通过双光子量子Rabi模型近似,并提出了一种简单的散射实验来探讨其基本性质。 特别地,我们识别出一种揭示选择规则的变化的驱动方案,其特征在于旋转波近似的击穿和从强度到超空间两光子相互作用的转变。 最后,我们表明,随着耦合强度接近塌陷点,在输出荧光光谱中可观察到窄光谱区域中的频率拥挤,从而铺平到固态装置中的光谱塌陷开始的直接观察的方式。

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