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Revealing nonclassicality beyond Gaussian states via a single marginal distribution

机译:通过单一边际分布揭示高斯状态以外的非经典性

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摘要

A standard method to obtain information on a quantum state is to measure marginal distributions along many different axes in phase space, which forms a basis of quantum-state tomography. We theoretically propose and experimentally demonstrate a general framework to manifest nonclassicality by observing a single marginal distribution only, which provides a unique insight into nonclassicality and a practical applicability to various quantum systems. Our approach maps the 1D marginal distribution into a factorized 2D distribution by multiplying the measured distribution or the vacuum-state distribution along an orthogonal axis. The resulting fictitious Wigner function becomes unphysical only for a nonclassical state; thus the negativity of the corresponding density operator provides evidence of nonclassicality. Furthermore, the negativity measured this way yields a lower bound for entanglement potential—a measure of entanglement generated using a nonclassical state with a beam-splitter setting that is a prototypical model to produce continuous-variable (CV) entangled states. Our approach detects both Gaussian and non-Gaussian nonclassical states in a reliable and efficient manner. Remarkably, it works regardless of measurement axis for all non-Gaussian states in finite-dimensional Fock space of any size, also extending to infinite-dimensional states of experimental relevance for CV quantum informatics. We experimentally illustrate the power of our criterion for motional states of a trapped ion, confirming their nonclassicality in a measurement-axis–independent manner. We also address an extension of our approach combined with phase-shift operations, which leads to a stronger test of nonclassicality, that is, detection of genuine non-Gaussianity under a CV measurement.
机译:获取有关量子态信息的标准方法是测量沿相空间中许多不同轴的边际分布,这是量子态层析成像的基础。我们在理论上提出并通过实验证明了通过仅观察单个边际分布来体现非经典性的通用框架,该框架为非经典性提供了独特的见识,并为各种量子系统提供了实际适用性。我们的方法通过乘以沿正交轴的测量分布或真空状态分布,将一维边际分布映射为因式分解的二维分布。虚构的维格纳函数仅对于非经典状态变得不物理。因此,相应密度算子的负性提供了非经典性的证据。此外,以这种方式测量的负性会产生纠缠潜力的下限-一种使用非经典状态与分束器设置生成的纠缠量度,分束器设置是产生连续变量(CV)纠缠态的原型模型。我们的方法以可靠且有效的方式检测高斯和非高斯非经典状态。值得注意的是,对于任何大小的有限维Fock空间中的所有非高斯态,它都与测量轴无关,并且可以扩展到与CV量子信息学相关的实验的无限维状态。我们以实验方式说明了我们对于被困离子运动状态的判据的能力,并以与测量轴无关的方式确认了其非经典性。我们还将解决方法扩展与相移操作相结合的问题,这将导致对非经典性的更强测试,即在CV测量下检测真正的非高斯性。

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