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Cold atoms in light fields: from free space optical lattices to multimode optical cavities

机译:光场中的冷原子:从自由空间光学晶格到多模光学腔

摘要

The electromagnetic mode density of the vacuum can be dramaticallyudmodified by the presence of an optical resonator. In the strong couplingudregime, spontaneous emission in a cavity becomes a reversible process andudthe intracavity photon number undergoes Rabi oscillations. We load upudto 200x10^3 ^133Cs atoms into a nearly confocal lossy cavity and reach theudcollective strong coupling regime. Normal mode splitting, the hallmark of this regime, is observed and cooperativities up to C_coll = (186±5) are measured. In a second experiment we investigate for the first timeudthe multi-mode character of the coupled cavity-atom system. In a confocaludcavity the higher-order transverse cavity modes are degenerate in frequency and accessible to the spontaneous emission of the atomic ensemble.udWe observe an increase of the coupling constant measured via modal decomposed transmission analysis, which could be attributed toudthe presence of the higher-order modes. Normal mode splitting proportional to the square root of the atom number was visible for all of theuddifferent mode components. Furthermore, we observe a redistribution of the relative weights in the modal transmission composition, which scales with the atom number in the cavity mode. udIn a second set of experiments, ^87Rb atoms were loaded into a dissipativeudlin ⊥ lin lattice. By driving the lattice with a biharmonic force, transport can be observed when the systems symmetries are broken: the so called ratchet effect. Research in this area is concerned with the appearanceudof current reversals. We were able to identify dissipation related symmetry breaking as the underlying cause of an observed current reversal, which occurs as a function of the driving frequency. Furthermore, in audsecond experiment, we use the ratchet effect as a probe of the optical potential depths. We show that an oscillating force with a frequency far above any other system-inherent timescale, can be used to renormalizeudthe optical potential. The ^87Rb atoms experience an average position dependent force, which becomes controllable over the amplitude of theudapplied driving.
机译:真空的电磁模式密度可以通过光学谐振器的存在而大大改变。在强耦合 udregime中,腔中的自发发射变为可逆过程,并且腔内光子数经历Rabi振荡。我们将 udto 200x10 ^ 3 ^ 133Cs原子加载到一个几乎共焦的有损腔中,并达到 udcollective强耦合态。观察到正常模式分裂,这是该机制的标志,并测量了高达C_coll =(186±5)的合作能力。在第二个实验中,我们首次研究了耦合腔原子系统的多模特性。在共焦 udvity中,高阶横向腔模在频率上退化并且可以自发发射到原子团。 ud我们观察到通过模态分解透射分析测得的耦合常数增加,这可能是由于 udthe高阶模式的存在。对于所有不同模式的分量,都可以看到与原子序数的平方根成比例的普通模式分裂。此外,我们观察到模态传输成分中相对权重的重新分布,该模量与腔模中的原子数成比例。在第二组实验中,^ 87Rb原子被加载到耗散的udlin lin lin晶格中。通过用双谐波力驱动晶格,可以在系统对称性破坏时观察到传输:所谓的棘轮效应。该领域的研究涉及电流反转的外观 ud。我们能够将与耗散相关的对称性破坏识别为观察到的电流反转的根本原因,该电流反转是驱动频率的函数。此外,在第二实验中,我们使用棘轮效应作为光势深度的探针。我们表明,具有远高于任何其他系统固有时间标度的频率的振荡力可用于使光势归一化。 ^ 87Rb原子受到平均位置相关的力,该力在未施加的驱动的振幅上变得可控。

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  • 作者

    Wickenbrock A;

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  • 年度 2012
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  • 原文格式 PDF
  • 正文语种 eng
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