Liang Yao, Tsai Din Ping, Kivshar Yuri
Department of Electrical Engineering, <a href="https://ror.org/03q8dnn23">City University of Hong Kong</a>, Kowloon, Hong Kong SAR, China.
State Key Laboratory of Terahertz and Millimeter Waves, <a href="https://ror.org/03q8dnn23">City University of Hong Kong</a>, Kowloon, Hong Kong SAR, China.
Phys Rev Lett. 2024 Aug 2;133(5):053801. doi: 10.1103/PhysRevLett.133.053801.
The physics of bound states in the continuum (BICs) allows the design and demonstration of optical resonant structures with large values of the quality factor (Q factor) by employing dielectric structures with low losses. However, BIC is a general wave phenomenon that should be observed in many systems, including the metal-dielectric structures supporting surface plasmon polaritons where optical resonances are hindered by losses. Here we suggest and develop a comprehensive strategy to achieve high-Q resonances in plasmonic metasurfaces by effectively tailoring the resonant modes from local to nonlocal regimes, thus transitioning from quasi-isolated localized resonances to extended resonant modes involving strong interaction among neighboring structure metaunits.
连续域束缚态(BICs)的物理学原理允许通过使用低损耗的介电结构来设计和展示具有高品质因数(Q 因子)的光学谐振结构。然而,BIC 是一种普遍的波动现象,应该在许多系统中都能观察到,包括支持表面等离激元极化激元的金属 - 介电结构,在这种结构中光学谐振会受到损耗的阻碍。在此,我们提出并开发了一种全面的策略,通过有效地将谐振模式从局部区域调整到非局部区域,从而在等离子体超表面中实现高 Q 谐振,进而从准孤立的局域谐振转变为涉及相邻结构元之间强相互作用的扩展谐振模式。