We analyze the creation of spin squeezed atomic ensembles by simultaneousdispersive interactions with several optical frequencies. A judicious choice ofoptical parameters enables optimization of an interferometric detection schemethat suppresses inhomogeneous light shifts and keeps the interferometeroperating in a balanced mode that minimizes technical noise. We show that whenthe atoms interact with two-frequency light tuned to cycling transitions thedegree of spin squeezing $\xi^2$ scales as $\xi^2\sim 1/d$ where $d$ is theresonant optical depth of the ensemble. In real alkali atoms there are losschannels and the scaling may be closer to $\xi^2\sim 1/\sqrt d.$ Neverthelessthe use of two-frequencies provides a significant improvement in the degree ofsqueezing attainable as we show by quantitative analysis of non-resonantprobing on the Cs D1 line. Two alternative configurations are analyzed: aMach-Zehnder interferometer that uses spatial interference, and an interactionwith multi-frequency amplitude modulated light that does not require a spatialinterferometer.
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机译:我们通过与几个光学频率的同时色散相互作用来分析自旋压缩的原子团的创建。明智地选择光学参数可以优化干涉检测方案,从而抑制不均匀的光偏移,并使干涉仪保持在平衡模式下工作,从而将技术噪声降至最低。我们表明,当原子与调谐到循环跃迁的两频光相互作用时,自旋压缩度的压缩程度为\\ xi ^ 2 \ sim 1 / d $,其中$ d $是集合的共振光学深度。在实际的碱原子中,存在损耗通道,并且缩放比例可能更接近$ \ xi ^ 2 \ sim 1 / \ sqrt d。尽管如此,使用双频可以显着改善可达到的压缩程度,正如我们通过定量分析得出的Cs D1线上的非共振探测。分析了两种替代配置:使用空间干涉的马赫曾德尔干涉仪,以及与不需要空间干涉仪的多频调幅光的相互作用。
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