Cavity Protected Multifrequency Polaritons in a Cold Atomic System

Pierre-Antoine Bourdel, Mohamed Baghdad, S. Schwartz, Constance Poulain, J. Reichel, R. Long
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Abstract

Controlling and characterizing entanglement in large quantum systems is an exciting challenge of modern physics. Along this line, we have built a CQED (Cavity Quantum Electrodynamics) platform where cold rubidium atoms are strongly coupled to a fiber-based Fabry-Perot cavity under a high-numerical aperture lens. The cavity is used to create collective interactions between the atomic qubits, and generate multiparticle entanglement, while the microscope is meant to allow for single-qubit manipulation and readout. Increasing the number of qubits of a quantum system without decreasing its coherence is one of the main achievments necessary to fulfil the promises of quantum technologies. Indeed, systems with many qubits are often inhomogeneous in frequency and subjected to decoherence. In inhomogeneous light-matter coupled systems, all eigenstates have a photonic component, contrary to homogeneous systems for which only the two polaritons have a photonic component. Therefore, the distribution of the photonic excitation among the eigenstates is a way to apprehend coherence. In our experiment, frequency inhomogeneity comes from the strong position-dependent lightshift induced by our trapping intra-cavity lattice. Thus we can tune the amount of inhomogeneity by changing the depth of this lattice. By tuning the number of atoms, and thus the collective coupling to the cavity, and by measuring an experimental quantity quantity analog to the photonic weight distribution, we observed a smooth transition between two different regimes: For low collective couplings, the photonic weight is distributed among many eigenstates, because of the frequency inhomogeneity. For higher collective couplings, the photonic weight is held by the sole two polaritons, and the coherence is retrieved in spite of the inhomogeneities. This is a ”cavity protection” effect, as theoretically described in [1, 2, 3] and previously experimentally observed in [4,5]. To our knowledge, this is the first experiment that finely characterizes this transition with a mesoscopic number of qubits (a few tens to hundreds), leveraging the strong coupling of each individual atom. Speaker sciencesconf.org:coolme2021:376109 Finally, using the high sensitivity of the light-shifted atomic frequency to the 1560nm dipole light power, we modulate the polariton frequencies very efficiently. We thus demonstrate a frequency modulated Rabi splitting, which increases the number of available frequencies of the coupled system while preserving its coherence thanks to cavity protection. Such spectral shaping of the polaritons could have applications for quantum memories and quantum communications. R. Houdré et al., PRA 53(4) (1996) Z. Kurucz et al., PRA 83, 053852 (2011) I. Diniz et al., PRA 84, 063810 (2011) S. Putz et al., Nat. Phys., 10(10) (2014) T. Zhong et al., Nat. Commun., 8, 14107 (2017)
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冷原子系统中腔保护的多频极化子
控制和表征大量子系统中的纠缠是现代物理学的一个令人兴奋的挑战。沿着这条线,我们已经建立了一个CQED(腔量子电动力学)平台,冷铷原子在高数值孔径透镜下与基于纤维的Fabry-Perot腔强耦合。空腔用于在原子量子位之间产生集体相互作用,并产生多粒子纠缠,而显微镜旨在允许单量子位操纵和读出。增加量子系统的量子比特数量而不降低其相干性是实现量子技术承诺所必需的主要成就之一。事实上,拥有许多量子位元的系统在频率上往往是不均匀的,并且会受到退相干的影响。在非均匀光-物质耦合系统中,所有本征态都有光子分量,而在均匀系统中,只有两个极化子有光子分量。因此,光子激发在本征态中的分布是理解相干性的一种方式。在我们的实验中,频率不均匀性来自于我们的捕获腔内晶格引起的强位置相关光移。因此,我们可以通过改变晶格的深度来调整不均匀性的数量。通过调整原子的数量,从而使集体耦合到腔中,并通过测量与光子重量分布类似的实验量,我们观察到两种不同状态之间的平滑过渡:对于低集体耦合,由于频率不均匀性,光子重量分布在许多本征态中。对于更高的集体耦合,光子重量由唯一的两个极化子保持,尽管存在不均匀性,但相干性被恢复。这是一种“空腔保护”效应,理论描述在[1,2,3]中,先前的实验观察在[4,5]中。据我们所知,这是第一个利用每个原子的强耦合,用介观数量的量子比特(几十到几百个)精细地表征这种转变的实验。最后,利用光移原子频率对1560nm偶极子光功率的高灵敏度,我们非常有效地调制了极化子频率。因此,我们展示了频率调制的拉比分裂,它增加了耦合系统的可用频率数量,同时由于腔保护而保持了其相干性。这种极化子的谱形可以应用于量子存储器和量子通信。R. houdr等人,物理学报53(4)(1996)Z. Kurucz等人,物理学报83,053852 (2011)I. Diniz等人,物理学报84,063810 (2011)S. Putz等人,物理学报。科学通报,10(10)(2014)。农业学报,8,14107 (2017)
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