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A sub-ensemble theory of ideal quantum measurement processes

机译:亚合奏理论的理想量子测量过程

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In order to elucidate the properties currently attributed to ideal measurements, one must explain how the concept of an individual event with a well-defined outcome may emerge from quantum theory which deals with statistical ensembles, and how different runs issued from the same initial state may end up with different final states. This so-called "measurement problem" is tackled with two guidelines. On the one hand, the dynamics of the macroscopic apparatus A coupled to the tested system S is described mathematically within a standard quantum formalism, where "q-probabilities" remain devoid of interpretation. On the other hand, interpretative principles, aimed to be minimal, are introduced to account for the expected features of ideal measurements. Most of the five principles stated here, which relate the quantum formalism to physical reality, are straightforward and refer to macroscopic variables. The process can be identified with a relaxation of S + A to thermodynamic equilibrium, not only for a large ensemble epsilon of runs but even for its sub-ensembles. The different mechanisms of quantum statistical dynamics that ensure these types of relaxation are exhibited, and the required properties of the Hamiltonian of S A are indicated. The additional theoretical information provided by the study of sub-ensembles remove Schrodinger's quantum ambiguity of the final density operator for epsilon which hinders its direct interpretation, and bring out a commutative behaviour of the pointer observable at the final time. The latter property supports the introduction of a last interpretative principle, needed to switch from the statistical ensembles and sub-ensembles described by quantum theory to individual experimental events. It amounts to identify some formal "q-probabilities" with ordinary frequencies, but only those which refer to the final indications of the pointer. The desired properties of ideal measurements, in particular the uniqueness of the result for each individual run of the ensemble and von Neumann's reduction, are thereby recovered with economic interpretations. The status of Born's rule involving both A and S is re-evaluated, and contextuality of quantum measurements is made obvious. (C) 2016 Elsevier Inc. All rights reserved.
机译:为了阐明目前归因于理想测量的性质,必须解释具有明确定义结果的单个事件的概念可以从量子理论中出现,这些概况涉及统计集合,以及从相同的初始状态发出的不同运行可能最终结束不同的最终状态。这种所谓的“测量问题”是用两个指导方针解决的。一方面,在数学上耦合到测试系统S的宏观设备A的动态在标准量子形式中描述,其中“q概率”仍然没有解释。另一方面,旨在最小化的解释性原则被介绍占理想测量的预期特征。这里规定的大部分原则,将量子形式主义与物理现实相关,是直接的,并指的是宏观变量。该过程可以通过S + A的放松来识别热力学平衡,不仅用于运行的大型epsilon,而且甚至是其子合奏。展示了确保这些类型放松的量子统计动态的不同机制,并指出了S A的哈密顿的所需性质。副作用的研究提供的额外理论信息删除了Schrodinger的最终密度算子的εuthedepsilon的量子模糊,其阻碍了其直接解释,并在最终时间发出了指针观察的换向行为。后一属性支持引入最后一个解释性原则,需要从量子理论描述的统计集合和子节奏到各个实验事件。它相当于识别具有普通频率的一些正式的“Q概率”,但只有那些指指针的最终指示的“Q-概率”。因此,通过经济解释恢复了理想测量的理想测量的所需性质,特别是每个单独的常规运行的结果的唯一性,从而恢复了经济解释。涉及A和S涉及A和S的诞生规则的地位,并且量子测量的上下文性明显。 (c)2016年Elsevier Inc.保留所有权利。

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