Campione Salvatore, Basilio Lorena I, Warne Larry K, Sinclair Michael B
Opt Express. 2015 Feb 9;23(3):2293-307. doi: 10.1364/OE.23.002293.
In this paper we describe a methodology for tailoring the design of metamaterial dielectric resonators, which represent a promising path toward low-loss metamaterials at optical frequencies. We first describe a procedure to decompose the far field scattered by subwavelength resonators in terms of multipolar field components, providing explicit expressions for the multipolar far fields. We apply this formulation to confirm that an isolated high-permittivity dielectric cube resonator possesses frequency separated electric and magnetic dipole resonances, as well as a magnetic quadrupole resonance in close proximity to the electric dipole resonance. We then introduce multiple dielectric gaps to the resonator geometry in a manner suggested by perturbation theory, and demonstrate the ability to overlap the electric and magnetic dipole resonances, thereby enabling directional scattering by satisfying the first Kerker condition. We further demonstrate the ability to push the quadrupole resonance away from the degenerate dipole resonances to achieve local behavior. These properties are confirmed through the multipolar expansion and show that the use of geometries suggested by perturbation theory is a viable route to achieve purely dipole resonances for metamaterial applications such as wave-front manipulation with Huygens' metasurfaces. Our results are fully scalable across any frequency bands where high-permittivity dielectric materials are available, including microwave, THz, and infrared frequencies.
在本文中,我们描述了一种定制超材料介质谐振器设计的方法,这是迈向光频低损耗超材料的一条有前景的途径。我们首先描述一种程序,根据多极场分量分解亚波长谐振器散射的远场,给出多极远场的显式表达式。我们应用此公式来确认一个孤立的高介电常数介质立方体谐振器具有频率分离的电偶极和磁偶极共振,以及在靠近电偶极共振处的磁四极共振。然后,我们按照微扰理论建议的方式,在谐振器几何结构中引入多个介质间隙,并证明能够使电偶极和磁偶极共振重叠,从而通过满足第一个克尔条件实现定向散射。我们进一步证明能够将四极共振推离简并偶极共振以实现局域行为。这些特性通过多极展开得到证实,表明使用微扰理论建议的几何结构是实现超材料应用(如用惠更斯超表面进行波前操纵)纯偶极共振的可行途径。我们的结果在任何有高介电常数介质材料可用的频段上都完全可扩展,包括微波、太赫兹和红外频率。