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从量子概率到量子振幅。

From Quantum Probabilities to Quantum Amplitudes.

作者信息

Martínez-Garaot Sofia, Pons Marisa, Sokolovski Dmitri

机构信息

Departamento de Química-Física, Universidad del País Vasco, UPV/EHU, 48940 Leioa, Spain.

Departamento de Física Aplicada I, Universidad del País Vasco, UPV-EHU, 48013 Bilbao, Spain.

出版信息

Entropy (Basel). 2020 Dec 8;22(12):1389. doi: 10.3390/e22121389.

Abstract

The task of reconstructing the system's state from the measurements results, known as the Pauli problem, usually requires repetition of two successive steps. Preparation in an initial state to be determined is followed by an accurate measurement of one of the several chosen operators in order to provide the necessary "Pauli data". We consider a similar yet more general problem of recovering Feynman's transition (path) amplitudes from the results of at least three consecutive measurements. The three-step histories of a pre- and post-selected quantum system are subjected to a type of interference not available to their two-step counterparts. We show that this interference can be exploited, and if the intermediate measurement is "fuzzy", the path amplitudes can be successfully recovered. The simplest case of a two-level system is analysed in detail. The "weak measurement" limit and the usefulness of the path amplitudes are also discussed.

摘要

从测量结果重建系统状态的任务,即所谓的泡利问题,通常需要重复两个连续步骤。首先在一个待确定的初始状态下进行制备,然后对几个选定算符之一进行精确测量,以提供必要的“泡利数据”。我们考虑一个类似但更具普遍性的问题,即从至少三次连续测量的结果中恢复费曼跃迁(路径)振幅。一个预选和后选量子系统的三步历史经历了一种其两步对应情况所不具备的干涉类型。我们表明这种干涉可以被利用,并且如果中间测量是“模糊的”,路径振幅就能被成功恢复。详细分析了两能级系统的最简单情况。还讨论了“弱测量”极限以及路径振幅的有用性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7982/7763750/8b1ffdeb8abd/entropy-22-01389-g001.jpg

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