Customizable dual-resonance sensing empowered by coupled quasi-bound states in the continuum

Xiao-Qing Luo, Yaojie Zhou, Qinke Liu, Zhendong Lu, Sha Chen, Yan Li, W.M. Liu
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Abstract

The quasi-bound states in the continuum (QBIC) have drawn increasing attention in optical metasurfaces derived from their ultrahigh quality factors, and show the utility to enhance the sensitivity of optical sensing. However, conventional single-resonance sensing may be inaccurate and unreliable, and then the dual-resonance sensing governed by the coupled QBIC is desired but remains elusive. Here, we show that the coupled QBIC modes can be leveraged to unfold dual-resonance refractive index sensing in the hybrid all-dielectric metasurface. Specifically, it is revealed that the toroidal dipole mode can be realized with strong electric field enhancement, enabling the implementation of anapole mode in the telecom short-wavelength band (1460–1530 nm). Under different linearly polarized illuminations, the dual symmetry-protected QBIC modes dominated by the electric quadrupole resonance can be fulfilled in the telecom extended-wavelength band (1360–1460 nm). Within this framework, the polarization-dependent dual symmetry-protected QBIC modes selectively coupled with the toroidal dipole mode or the anapole mode can not only uncover the transformation from Fano resonance to analog of electromagnetically induced transparency, but also manifest two types of high-sensitivity dual-resonance refractive index sensing in the telecom extended-wavelength and short-wavelength bands. The dual-resonance refractive index sensing can also be extended to telecom long-wavelength band (1565–1625 nm) and ultra-long-wavelength band (1625–1675 nm) with enhanced sensitivity. These results offer exploration potential for multi-channel sensing, optical modulators, and slow-light devices.
利用连续体中的耦合准约束态实现可定制的双共振传感
连续体中的准约束态(QBIC)因其超高的品质因数而在光学超表面中引起越来越多的关注,并显示出提高光学传感灵敏度的实用性。然而,传统的单共振传感可能不准确、不可靠,因此人们希望采用耦合 QBIC 的双共振传感技术,但这一技术仍难以实现。在这里,我们展示了如何利用耦合 QBIC 模式在混合全介质元表面中展开双共振折射率传感。具体来说,我们发现环偶极子模式可以在强电场增强的情况下实现,从而在电信短波段(1460-1530 nm)实现无偶极子模式。在不同的线性极化光照下,由电四极共振主导的双对称保护 QBIC 模式可以在电信扩展波长波段(1360-1460 nm)内实现。在此框架内,偏振相关的双对称保护 QBIC 模式选择性地与环偶极子模式或无极子模式耦合,不仅能揭示从法诺共振到类似电磁诱导透明的转变,还能在电信扩展波长和短波长波段实现两种类型的高灵敏度双共振折射率传感。双共振折射率传感还可以扩展到电信长波长波段(1565-1625 nm)和超长波长波段(1625-1675 nm),并提高灵敏度。这些成果为多通道传感、光调制器和慢光器件提供了探索潜力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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