从费曼的量子电动力学方法中获得了对某些光学系统行为的见解

M. Mansuripur
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引用次数: 2

摘要

Richard Feynman的路径积分方法是基于这样一个基本假设:一个系统从一个点出发,到达一个点,采用所有可能的路径,从一个点到一个点,每个路径都有自己的(复杂的)概率幅度。所有这些路径上的振幅之和,然后产生系统从变量变量开始最终到达变量变量的总体概率振幅。我们将费曼方法应用于几个实际感兴趣的光学系统,并讨论了该方法的细微差别以及预测结果与经典光学理论一致或不一致的实例。例子包括分束器的性质,单光子通过马赫-曾达和萨格纳克干涉仪,电和磁偶极子散射,互易性,时间反演对称性,光学定理,Ewald-Oseen消光定理,远场衍射,以及被称为洪瓯-曼德尔效应的双光子干涉现象。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Insights into the behavior of certain optical systems gleaned from Feynman's approach to quantum electrodynamics
Richard Feynman’s method of path integrals is based on the fundamental assumption that a system starting at a point 𝐴𝐴 and arriving at a point 𝐵𝐵 takes all possible paths from 𝐴𝐴 to 𝐵𝐵, with each path contributing its own (complex) probability amplitude. The sum of the amplitudes over all these paths then yields the overall probability amplitude that the system starting at 𝐴𝐴 would end up at 𝐵𝐵. We apply Feynman’s method to several optical systems of practical interest and discuss the nuances of the method as well as instances where the predicted outcomes agree or disagree with those of classical optical theory. Examples include the properties of beam-splitters, passage of single photons through Mach-Zehnder and Sagnac interferometers, electric and magnetic dipole scattering, reciprocity, time-reversal symmetry, the optical theorem, the Ewald-Oseen extinction theorem, far field diffraction, and the two-photon interference phenomenon known as the Hong-Ou-Mandel effect.
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