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混合电路腔量子电动力学与微机械谐振器。

Hybrid circuit cavity quantum electrodynamics with a micromechanical resonator.

机构信息

Low Temperature Laboratory, Aalto University, PO Box 15100, FI-00076 Aalto, Finland.

出版信息

Nature. 2013 Feb 14;494(7436):211-5. doi: 10.1038/nature11821.

Abstract

Hybrid quantum systems with inherently distinct degrees of freedom have a key role in many physical phenomena. Well-known examples include cavity quantum electrodynamics, trapped ions, and electrons and phonons in the solid state. In those systems, strong coupling makes the constituents lose their individual character and form dressed states, which represent a collective form of dynamics. As well as having fundamental importance, hybrid systems also have practical applications, notably in the emerging field of quantum information control. A promising approach is to combine long-lived atomic states with the accessible electrical degrees of freedom in superconducting cavities and quantum bits (qubits). Here we integrate circuit cavity quantum electrodynamics with phonons. Apart from coupling to a microwave cavity, our superconducting transmon qubit, consisting of tunnel junctions and a capacitor, interacts with a phonon mode in a micromechanical resonator, and thus acts like an atom coupled to two different cavities. We measure the phonon Stark shift, as well as the splitting of the qubit spectral line into motional sidebands, which feature transitions between the dressed electromechanical states. In the time domain, we observe coherent conversion of qubit excitation to phonons as sideband Rabi oscillations. This is a model system with potential for a quantum interface, which may allow for storage of quantum information in long-lived phonon states, coupling to optical photons or for investigations of strongly coupled quantum systems near the classical limit.

摘要

具有固有不同自由度的混合量子系统在许多物理现象中起着关键作用。众所周知的例子包括腔量子电动力学、囚禁离子以及固态中的电子和声子。在这些系统中,强耦合使组成部分失去其个体特征,形成了修饰态,代表了一种集体动力学形式。混合系统不仅具有重要的基础性,还有实际应用,特别是在新兴的量子信息控制领域。一种很有前途的方法是将长寿命的原子态与超导腔和量子位(qubit)中的可访问电自由度相结合。在这里,我们将电路腔量子电动力学与声子结合起来。除了与微波腔耦合外,我们的超导传输子量子位由隧道结和电容器组成,与微机械谐振器中的声子模式相互作用,从而表现得像一个与两个不同腔耦合的原子。我们测量了声子斯塔克位移,以及量子位谱线分裂为运动边带,其特征是修饰机电态之间的跃迁。在时域中,我们观察到量子位激发到声子的相干转换,表现为边带拉比振荡。这是一个具有量子接口潜力的模型系统,它可能允许将量子信息存储在长寿命的声子态中,与光光子耦合,或者研究接近经典极限的强耦合量子系统。

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