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中国物理学会期刊

纳米结构单元内扰动调控q-BIC超表面的本征偏振

CSTR: 32037.14.aps.75.20251777

Intra-meta-atom perturbations for manipulating the intrinsic polarization of q-BIC metasurface

CSTR: 32037.14.aps.75.20251777
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  • 准连续域束缚态(quasi-bound states in the continuum, q-BIC)超表面具有高Q值和强局域场, 能够实现共振波长、振幅、相位及偏振等有效操控, 是实现高性能传感和光电子器件的理想平台. 现有q-BIC偏振调控多依赖旋转纳米结构单元或改变结构高度, 加工复杂且灵活性不足, 限制了其在偏振维度的多功能集成. 本研究提出了一种在纳米结构单元内部引入孔洞微扰的策略, 直接调控q-BIC的本征偏振模式. 研究通过耦合模理论和多极子分解解析了微扰改变结构单元局域介电常数及电偶极矩分布, 从而影响本征偏振方向的物理机制. 设计并制备了基于a-Si纳米柱二聚体的系列超表面样品, 通过改变孔洞数量及排布引入微扰. 仿真与实验结果表明, 随着孔洞数量增加, q-BIC的本征偏振方向能从初始0°发生顺时针偏转, 同时共振波长产生蓝移. 实验测得的偏振响应与仿真结果一致. 本文研究提供了一种简易、灵活的q-BIC偏振操控手段, 为发展紧凑型偏振转换、偏振测量与信息处理超表面开辟了新途径.

     

    Quasi-bound states in the continuum (q-BIC) supported by metasurfaces enable resonant modes with ultra-high quality factors, making them promising for nanophotonic applications. Manipulating the polarization of these modes, however, remains challenging. Conventional approaches rely on rotating the meta-atoms or varying their vertical geometry, which complicates fabrication and limits design flexibility. Here, we introduce an alternative strategy: embedding rectangular slots directly within the dielectric meta-atoms. This intra-unit perturbation locally modifies the permittivity distribution, thereby altering the optical response without requiring complex three-dimensional reconfiguration.
    The physical mechanism is analyzed using coupled-mode theory and multipole expansion. The intrinsic polarization direction is shown to be governed by the superposition of electric dipole moments in the dimer unit cell. Introducing slots into a nanorod reduces its effective polarizability, selectively modifying specific components of the dipole moment. As a result, the overall polarization axis can be rotated in a controlled manner. We experimentally realized this concept using amorphous-silicon nanorod dimers fabricated on quartz. The base q-BIC resonance was excited by rotating the rods by 12.5° to break in-plane symmetry. Through electron-beam lithography and dry etching, we introduced 0 to 3 slots per dimer in various arrangements. Polarization-resolved transmission spectroscopy is performed using a motorized rotating polarizer and a microscope-coupled spectrometer.
    Measurements reveal that increasing the number of slots in one rod from 0 to 2 progressively rotates the intrinsic polarization clockwise from 0°, accompanied by a blue shift of the resonance. For instance, samples with 0, 1, and 2 slots exhibited polarization angles of 0°, 162°, and 146°, respectively. When slots are added to both rods to restore approximate intra-unit symmetry (e.g., 3-slot designs), the polarization realigns closer to the unperturbed orientation. These results confirm that slot-based perturbations offer a reliable and lithographically accessible means to independently tailor both the polarization state and the spectral position of q-BIC resonances.
    This work demonstrates a straightforward and effective method for polarization engineering in high-Q metasurfaces, opening avenues for designing versatile polarization-sensitive devices such as tunable waveplates, polarimetric sensors, and compact polarization encoders in integrated photonic systems.

     

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