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arXiv 1702.00347quant-ph
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最优弱值测量:纯态

Optimal weak value measurements: Pure states

N. D. Hari Dass, R. Rajath Krishna, Sai Smruti Samantaray

摘要:

我们将Wootters和Fields最初给出的用于状态确定(断层扫描)的测量的\emph{optimality}的概念应用于\emph{pure states}的\emph{weak value tomography}。他们将测量定义为最优的,如果它们“最小化”统计误差的影响。由于技术原因,他们实际上最大化了状态平均信息,精确地量化为“错误量”的负对数。在本文中,我们优化的状态平均信息以及错误量。我们证明了,对于任意(有限)维的Hilbert空间,当后选择的基地是\emph{mutually unbiased}关于被测量的可观察的特征向量的弱值测量的品种是最佳的。我们证明了一些重要的结果表示时,通过弱值作为坐标的状态空间的几何。我们导出了N维情形下的Kaëhler势的表达式,并利用它给出了任意自旋情形的精确处理。

英文摘要:

We apply the notion of \emph{optimality} of measurements for state determination(tomography) as originally given by Wootters and Fields to \emph{weak value tomography} of \emph{pure states}. They defined measurements to be optimal if they 'minimised' the effects of statistical errors. For technical reasons they actually maximised the state averaged information, precisely quantified as the negative logarithm of 'error volume'. In this paper we optimise both the state averaged information as well as error volumes. We prove, for Hilbert spaces of arbitrary (finite) dimensionality, that varieties of weak value measurements are optimal when the post-selected bases are \emph{mutually unbiased} with respect to the eigenvectors of the observable being measured. We prove a number of important results about the geometry of state spaces when expressed through the weak values as coordinates. We derive an expression for the Kaëhler potential for the N-dimensional case with the help of which we give an exact treatment of the arbitrary-spin case.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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