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等离激元超表面通过光与晶格场相互作用的自旋轨道相互作用来操纵两个自旋分量。

Plasmonic metasurfaces manipulating the two spin components from spin-orbit interactions of light with lattice field generations.

作者信息

Zhang Ruirui, Gu Manna, Sun Rui, Zeng Xiangyu, Zhang Yuqin, Zhang Yu, Cheng Chen, Zhan Zijun, Chen Chao, Ren Xiaorong, He Changwei, Liu Chunxiang, Cheng Chuanfu

机构信息

College of Physics and Electronics, Shandong Normal University, Jinan, 250014, China.

School of Computer Science and Technology, Shandong University of Finance and Economics, Jinan, 250014, China.

出版信息

Nanophotonics. 2021 Dec 13;11(2):391-404. doi: 10.1515/nanoph-2021-0567. eCollection 2022 Jan.

Abstract

Artificial nanostructures in metasurfaces induce strong spin-orbit interactions (SOIs), by which incident circularly polarized light can be transformed into two opposite spin components. The component with an opposite helicity to the incident light acquires a geometric phase and is used to realize the versatile functions of the metasurfaces; however, the other component, with an identical helicity, is often neglected as a diffused background. Here, by simultaneously manipulating the two spin components originating from the SOI in plasmonic metasurfaces, independent wavefields in the primary and converted spin channels are achieved; the wavefield in the primary channel is controlled by tailoring the dynamic phase, and that in the converted channel is regulated by designing the Pancharatnam-Berry phase in concurrence with the dynamic phase. The scheme is realized by generating optical lattice fields with different topologies in two spin channels, with the metasurfaces composed of metal nanoslits within six round-apertures mimicking the multi-beam interference. This study demonstrates independent optical fields in a dual-spin channel based on the SOI effect in the metasurface, which provides a higher polarization degree of freedom to modify optical properties at the subwavelength scale.

摘要

超表面中的人工纳米结构会引发强烈的自旋轨道相互作用(SOI),通过这种相互作用,入射圆偏振光可以被转换为两个相反的自旋分量。与入射光螺旋度相反的分量会获得一个几何相位,并被用于实现超表面的多种功能;然而,另一个具有相同螺旋度的分量通常被视为漫射背景而被忽略。在此,通过同时操控表面等离激元超表面中源自SOI的两个自旋分量,在初级和转换自旋通道中实现了独立的波场;初级通道中的波场通过调整动态相位来控制,而转换通道中的波场则通过与动态相位协同设计潘查拉特纳姆 - 贝里相位来调节。该方案是通过在两个自旋通道中生成具有不同拓扑结构的光学晶格场来实现的,超表面由六个圆孔内的金属纳米狭缝组成,模拟了多光束干涉。这项研究展示了基于超表面中SOI效应的双自旋通道中的独立光场,这为在亚波长尺度上修改光学特性提供了更高的偏振自由度。

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