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Wave-particle duality in multi-path interferometers: General concepts and three-path interferometers

机译:多径干涉仪中的波粒对偶性:一般概念和三径干涉仪

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摘要

For two-path interferometers, the which-path predictability P and the fringe visibility V are familiar quantities that are much used to talk about wave-particle duality in a quantitative way. We discuss several candidates that suggest themselves as generalizations P of P for multi-path interferometers, and treat the case of three paths in considerable detail. To each choice for the path knowledge P, the interference strength V - the corresponding generalization of V - is found by a natural, operational procedure. In experimental terms, it amounts to finding those equal-weight superpositions of the path amplitudes which maximize P for the emerging intensities. Mathematically speaking, one needs to identify a certain optimum one among the Fourier transforms of the state of the interfering quantum object. Wave-particle duality is manifest, inasmuch as P = 1 implies V = 0 and V = 1 implies P = 0, whatever definition is chosen. The possible values of the pair (P, V) are restricted to an area with corners at (P, V) = (0, 0), (P, V) = (1, 0), and (P, V) = (0, 1), with the shape of the border line from (1, 0) to (0, 1), depending on the particular choice for P and the induced definition of V.
机译:对于两径干涉仪,哪一条路径的可预测性P和条纹的可见性V是很熟悉的量,通常用于定量讨论波粒对偶。我们讨论了几种候选者,这些候选者建议将自己作为多路径干涉仪的P的推广P,并详细介绍三种路径的情况。对于路径知识P的每个选择,通过自然的操作过程来找到干扰强度V-V的对应概括。用实验术语来说,这等于找到路径振幅的等权重叠加,这些叠加使新兴强度的P最大化。从数学上讲,人们需要在干扰量子物体的状态的傅立叶变换中确定某个最佳值。波粒对偶性是明显的,因为无论选择什么定义,P = 1表示V = 0,而V = 1表示P = 0。该对(P,V)的可能值被限制在(P,V)=(0,0),(P,V)=(1,0)和(P,V)= (0,1),边界线的形状从(1,0)到(0,1),取决于对P的特定选择和对V的定义。

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