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能隙表面等离子体共振器中的无偶极子态

Anapole States in Gap-Surface Plasmon Resonators.

作者信息

Yezekyan Torgom, Zenin Vladimir A, Beermann Jonas, Bozhevolnyi Sergey I

机构信息

Centre for Nano Optics, University of Southern Denmark, Campusvej 55, DK-5230 Odense M, Denmark.

出版信息

Nano Lett. 2022 Aug 10;22(15):6098-6104. doi: 10.1021/acs.nanolett.2c01051. Epub 2022 Jul 22.

Abstract

Anapole states associated with the destructive interference between dipole and toroidal moments result in suppressed scattering accompanied by strongly enhanced near fields. In this work, we comprehensively examine the anapole state formation in metal-insulator-metal configurations supporting gap surface-plasmon (GSP) resonances that are widely used in plasmonics. Using multipole decomposition, we show that in contrast to the common case of dielectric particles with out-of-phase superposition of electric and toroidal dipoles anapole states in GSP resonators are formed due to the compensation of magnetic dipole moments. Unlike anapole states in dielectric particles, magnetic anapole states in GSP resonator does not provide a pronounced suppression of scattering, but it features huge electric field enhancement, which we verify by numerical simulations and two-photon luminescence measurements. This makes the GSP resonator configuration very promising for use in a wide range of applications, ranging from nonlinear harmonic generation to absorption enhancement and sensing.

摘要

与偶极矩和环形矩之间的相消干涉相关的无辐射态会导致散射受到抑制,并伴随着近场的强烈增强。在这项工作中,我们全面研究了在支持间隙表面等离子体激元(GSP)共振的金属-绝缘体-金属结构中无辐射态的形成,这种结构在等离子体学中被广泛使用。通过多极分解,我们表明,与电偶极和环形偶极异相叠加的普通电介质粒子情况不同,GSP谐振器中的无辐射态是由于磁偶极矩的补偿而形成的。与电介质粒子中的无辐射态不同,GSP谐振器中的磁无辐射态不会显著抑制散射,但它具有巨大的电场增强,我们通过数值模拟和双光子发光测量验证了这一点。这使得GSP谐振器结构在从非线性谐波产生到吸收增强和传感等广泛应用中非常有前景。

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