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中国物理学会期刊

手性核-介质层-银同心球结构的手性力学响应与近场光学特性

Chiral Optomechanical Effects and Near-Field Optical Properties of Chiral Core–Dielectric–Ag Concentric Sphere Structures

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  • 手性光学在生物传感与光学操控等领域具有广阔的应用前景,但天然手性材料的光学响应弱,而通过设计人工手性微纳结构可显著增强手性光学响应.本文对比纯手性介质球与外裹单层银壳或者介质壳的同心球结构,发现手性核-介质层-银壳同心球结构通过引入介质层与银壳耦合,成功在近红外波段同时实现了光学扭矩与手性密度的显著增强.光学扭矩的增强意味着该结构可被光场有效操控,而手性密度的增强意味着结构可产生强手性近场,作为平台增强附近手性物质的响应.进一步研究表明该结构银壳过厚时会屏蔽内部手性响应,增大手性核的相对介电常数则会抑制电多极共振;介质层对结构手性响应的增强存在最优厚度,增大介质层的折射率会在增强电偶极响应与磁多极响应的同时抑制电四极响应.本文系统探究了结构材料与几何参数对手性光学响应的调控规律,为发展生物相容的近红外手性光学器件以及手性粒子操控与传感平台提供了设计思路.

     

    Natural chiral materials have an intrinsically weak chiroptical response, limiting their use in high–sensitivity detection and optical manipulation. Although artificial chiral nanostructures can enhance this response, most studies focus on the visible range, where poor tissue penetration hinders biomedical applications. Core–shell architectures offer a versatile platform, but current designs mainly rely on complex geometric chirality, while structures based on intrinsic material chirality remain largely unexplored. Designing simple core–shell configurations that provide strong near‑infrared (NIR) chiroptical enhancement remains a challenge.
    Here, the finite element method is employed to calculate the scattering cross–section, optical torque, and optical chirality density. Four configurations are compared: a pure chiral sphere, a chiral core with a dielectric shell (chiral@dielectric), a chiral core with an Ag shell (chiral@Ag), and the full three‑layer chiral core–dielectric–Ag shell concentric sphere (chiral@dielectric@Ag). A systematic parametric study is performed to reveal the tuning rules of the chiral optical response.
    The results show that the proposed three‑layer structure simultaneously achieves significant enhancement of both optical torque and optical chirality density in the NIR band. Compared with chiral@Ag, the dielectric layer shifts the enhanced response to the NIR region and improves biocompatibility. The parametric study reveals key tuning rules: an excessively thick Ag shell suppresses the internal chiral response; increasing the core permittivity red–shifts the electric multipole resonances; the dielectric spacer has an optimal thickness that maximizes the chiroptical enhancement; and increasing the spacer refractive index red‑shifts all resonances and differentially affects the intensities of the electric dipole, magnetic multipole, and electric quadrupole responses.
    In conclusion, the proposed chiral@dielectric@Ag concentric sphere structure extends the enhanced chiroptical response to the NIR region while enhancing both optical torque and chirality density. The design is structurally simple, biocompatible, and provides new strategies for optical sorting and precise manipulation of chiral particles.

     

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