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首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Microwave-induced amplitude- and phase-tunable qubit-resonator coupling in circuit quantum electrodynamics
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Microwave-induced amplitude- and phase-tunable qubit-resonator coupling in circuit quantum electrodynamics

机译:电路量子电动力学中的微波感应振幅和相位可调量子比特谐振器耦合

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摘要

In the circuit quantum electrodynamics architecture, both the resonance frequency and the coupling of superconducting qubits to microwave field modes can be controlled via external electric and magnetic fields to explore qubit-photon dynamics in a wide parameter range. Here, we experimentally demonstrate and analyze a scheme for tuning the coupling between a transmon qubit and a microwave resonator using a single coherent drive tone. We treat the transmon as a three-level system, with the qubit subspace defined by the ground and the second excited states. If the drive frequency matches the difference between the resonator and the qubit frequencies, a Jaynes-Cummings-type interaction is induced, which is tunable in both amplitude and phase. We show that coupling strengths of about 10 MHz can be achieved in our setup, limited only by the anharmonicity of the transmon qubit. This scheme has been successfully used to generate microwave photons with a controlled temporal shape [M. Pechal et al., Phys. Rev. X 4, 041010 (2014)] and can be directly implemented with superconducting quantum devices featuring larger anharmonicity for higher coupling strengths.
机译:在电路量子电动力学体系结构中,可以通过外部电场和磁场控制共振频率以及超导量子位与微波场模式的耦合,从而在较宽的参数范围内探索量子位光子动力学。在这里,我们实验性地演示和分析了一种方案,该方案使用单个相干驱动音来调谐跨量子比特与微波谐振器之间的耦合。我们将transmon视为三级系统,其qubit子空间由基态和第二个激发态定义。如果驱动频率与谐振器和量子位频率之间的差相匹配,则会产生Jaynes-Cummings型相互作用,该相互作用在幅度和相位上都是可调的。我们表明,在我们的设置中可以达到大约10 MHz的耦合强度,仅受transmon量子位的非谐性限制。该方案已成功用于产生具有受控时间形状的微波光子[M. Pechal等,Phys。 [Rev. X 4,041010(2014)],并且可以直接使用具有更大非谐性的超导量子器件实现更高的耦合强度。

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