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平面手性纳米天线阵列的晶格和局域等离子体共振引起的自旋相关发射。

Spin-Dependent Emission from Arrays of Planar Chiral Nanoantennas Due to Lattice and Localized Plasmon Resonances.

机构信息

COBRA Research Institute, Eindhoven University of Technology , 5600 MB Eindhoven, The Netherlands.

Center for Nanophotonics, FOM Institute AMOLF , Science Park 104, 1098 XG Amsterdam, The Netherlands.

出版信息

ACS Nano. 2016 Mar 22;10(3):3389-97. doi: 10.1021/acsnano.5b07231. Epub 2016 Feb 15.

Abstract

Chiral plasmonic nanoantennas manifest a strong asymmetric response to circularly polarized light. Particularly, the geometric handedness of a plasmonic structure can alter the circular polarization state of light emitted from nearby sources, leading to a spin-dependent emission direction. In past experiments, these effects have been attributed entirely to the localized plasmonic resonances of single antennas. In this work, we demonstrate that, when chiral nanoparticles are arranged in diffractive arrays, lattice resonances play a primary role in determining the spin-dependent emission of light. We fabricate 2D diffractive arrays of planar chiral metallic nanoparticles embedded in a light-emitting dye-doped slab. By measuring the polarized photoluminescence enhancement, we show that the geometric chirality of the array's unit cell induces a preferential circular polarization, and that both the localized surface plasmon resonance and the delocalized hybrid plasmonic-photonic mode contribute to this phenomenon. By further mapping the angle-resolved degree of circular polarization, we demonstrate that strong chiral dissymmetries are mainly localized at the narrow emission directions of the surface lattice resonances. We validate these results against a coupled dipole model calculation, which correctly reproduces the main features. Our findings demonstrate that, in diffractive arrays, lattice resonances play a primary role into the light spin-orbit effect, introducing a highly nontrivial behavior in the angular spectra.

摘要

手性等离子体纳米天线对圆偏振光表现出强烈的不对称响应。特别地,等离子体结构的几何手性可以改变来自附近光源的光的圆偏振状态,导致自旋相关的发射方向。在过去的实验中,这些效应完全归因于单个天线的局域等离子体共振。在这项工作中,我们证明了当手性纳米粒子排列在衍射阵列中时,晶格共振在确定光的自旋相关发射中起着主要作用。我们在发光染料掺杂平板中制造了二维衍射阵列的平面手性金属纳米粒子。通过测量偏振光致发光增强,我们表明阵列单元的几何手性诱导了优先的圆偏振,并且局域表面等离激元共振和离域混合等离子体光子模式都有助于这种现象。通过进一步绘制角度分辨的圆偏振度,我们证明了强手性不对称性主要集中在表面晶格共振的狭窄发射方向上。我们通过与偶极子模型计算进行了验证,该计算正确地再现了主要特征。我们的研究结果表明,在衍射阵列中,晶格共振在手性光的自旋轨道效应中起着主要作用,在角谱中引入了非常复杂的行为。

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