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Lectures on dynamical models for quantum measurements

机译:量子测量动力学模型讲座

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摘要

In textbooks, ideal quantum measurements are described in terms of the tested system only by the collapse postulate and Born's rule. This level of description offers a rather flexible position for the interpretation of quantum mechanics. Here we analyse an ideal measurement as a process of interaction between the tested system S and an apparatus A, so as to derive the properties postulated in textbooks. We thus consider within standard quantum mechanics the measurement of a quantum spin component ?_z by an apparatus A, being a magnet coupled to a bath. We first consider the evolution of the density operator of S+A describing a large set of runs of the measurement process. The approach describes the disappearance of the off-diagonal terms ("truncation") of the density matrix as a physical effect due to A, while the registration of the outcome has classical features due to the large size of the pointer variable, the magnetization. A quantum ambiguity implies that the density matrix at the final time can be decomposed on many bases, not only the one of the measurement. This quantum oddity prevents to connect individual outcomes to measurements, a difficulty known as the "measurement problem". It is shown that it is circumvented by the apparatus as well, since the evolution in a small time interval erases all decompositions, except the one on the measurement basis. Once one can derive the outcome of individual events from quantum theory, the so-called collapse of the wavefunction or the reduction of the state appears as the result of a selection of runs among the original large set. Hence nothing more than standard quantum mechanics is needed to explain features of measurements. The employed statistical formulation is advocated for the teaching of quantum theory.
机译:在教科书中,仅通过坍塌假设和伯恩定律就测试系统描述了理想的量子测量。这种描述水平为量子力学的解释提供了相当灵活的位置。在这里,我们将理想测量作为被测系统S与设备A之间相互作用的过程进行分析,以得出教科书中假定的属性。因此,我们考虑在标准的量子力学中,由设备A对量子自旋分量的测量,该设备是耦合至槽的磁体。我们首先考虑描述大量测量过程的S + A密度算符的演化。该方法将密度矩阵的非对角项(“截断”)的消失描述为由于A引起的物理效应,而由于指针变量的大小(磁化强度),结果的配准具有经典特征。量子歧义意味着最终时间的密度矩阵可以在许多基础上分解,而不仅仅是测量中的一个。这种量子奇异性阻止了将单个结果与测量联系起来,这一困难被称为“测量问题”。示出了它也被设备规避,因为在小时间间隔内的演变消除了所有分解,除了基于测量的分解之外。一旦人们可以从量子理论中得出单个事件的结果,那么,在原始大集合中选择游程的结果就会出现所谓的波函数崩溃或状态降低。因此,只需要标准量子力学来解释测量的特征即可。提倡采用统计公式进行量子理论的教学。

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