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Configuring the cancellation of optical near-fields

机译:配置消除光学近场

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The characteristic near-field behavior of electromagnetic fields is open to a variety of interpretations. In a classical sense the term 'near-field' can be taken to signify a region, sufficiently close to some primary or secondary source, that the onset of retardation features is insignificant; a quantum theoretic explanation might focus more on the large momentum uncertainty that operates at small distances. Together, both near-field and wave-zone (radiative) features are fully accommodated in a retarded resonance propagation tensor, within which each component individually represents one asymptotic limit - alongside a third term that is distinctly operative at distances comparable to the optical wavelength. The propagation tensor takes different forms according to the level of multipole involved in the signal production and detection. In this presentation the nature and symmetry properties of the retarded propagation tensor are explored with reference to various forms of electric interaction, and it is shown how a suitable arrangement of optical beams can lead to the complete cancellation of near-fields. The conditions for such behavior are fully determined and some important optical trapping applications are discussed.
机译:电磁场的特征性近场行为有多种解释。在传统意义上,术语“近场”可以用来表示一个区域,该区域足够接近某个主要或次要来源,延迟特征的出现是无关紧要的;量子理论的解释可能更着重于在小距离上运行的大动量不确定性。总之,近场和波区(辐射)特征都完全容纳在延迟的共振传播张量中,其中每个分量分别表示一个渐近极限-第三项在可与光波长相当的距离上明显起作用。传播张量根据信号产生和检测所涉及的多极水平而采取不同的形式。在本演示中,参考了各种形式的电相互作用来探索延迟传播张量的性质和对称性,并说明了光束的合适布置如何可以导致近场的完全抵消。完全确定了这种行为的条件,并讨论了一些重要的光阱应用。

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