arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2405.08086physics.opticsquant-ph
收藏

光学介质中的量子化螺旋度

Quantised helicity in optical media

Neel Mackinnon, Jörg B. Götte, Stephen M. Barnett, Niclas Westerberg

AI总结:

本文提出一种新的光学介质螺旋度定义,通过引入与物质极化和磁化相关的显式贡献解决对偶变换与本构关系的不相容问题,并揭示非守恒情形下螺旋度本征态间的振荡行为。

摘要:

我们提出了一种定义介质中光学螺旋度的新方法。我们的方法解决了同时将 $\mathbf{E}$ 与 $\mathbf{H}$ 以及 $\mathbf{D}$ 与 $\mathbf{B}$ 结合的对偶变换与线性本构关系不相容的问题。我们发现,介质中的螺旋度密度作为与对偶变换相关的守恒量,必须包含一个与物质极化和磁化相关的显式贡献,并且它可以自然地用系统的基本极化激发来表示。在螺旋度守恒的介质中,每个圆偏振激发携带明确定义的螺旋度。然而,在螺旋度不守恒的介质中,我们发现随时间变化的螺旋度可以被视为不同螺旋度本征态之间的振荡,类似于中微子振荡。在这里,我们明确研究了均匀且无损耗介质中的螺旋度,但我们相信,与其他选择不同,这种螺旋度可以很容易地推广到可能非均匀、有损耗、手性或非互易的介质。

英文摘要:

We present a new approach to the definition of optical helicity in a medium. Our approach resolves the problem that duality transformations which simultaneously combine $\mathbf{E}$ with $\mathbf{H}$ and $\mathbf{D}$ with $\mathbf{B}$ are incompatible with linear constitutive relations. We find that the helicity density in a medium, as the conserved quantity associated with duality transforms, must contain an explicit contribution associated with the polarisation and magnetisation of the matter, and that it can be expressed naturally in terms of the elementary polarised excitations of the system. In media for which the helicity is conserved, each circular excitation carries a well-defined helicity. However, in a medium for which the helicity is not conserved, we find that the time-varying helicity can be viewed in terms of oscillations between different helicity eigenstates, analogous to neutrino oscillations. Here we explicitly study the helicity in homogeneous and lossless media but we believe that, differently to other choices, this helicity is readily generalisable to media that may be inhomogeneous, lossy, chiral or nonreciprocal.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑