Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology, Daejeon 305-751, South Korea.
Nature. 2011 Feb 17;470(7334):369-73. doi: 10.1038/nature09776.
Controlling the electromagnetic properties of materials, going beyond the limit that is attainable with naturally existing substances, has become a reality with the advent of metamaterials. The range of various structured artificial 'atoms' has promised a vast variety of otherwise unexpected physical phenomena, among which the experimental realization of a negative refractive index has been one of the main foci thus far. Expanding the refractive index into a high positive regime will complete the spectrum of achievable refractive index and provide more design flexibility for transformation optics. Naturally existing transparent materials possess small positive indices of refraction, except for a few semiconductors and insulators, such as lead sulphide or strontium titanate, that exhibit a rather high peak refractive index at mid- and far-infrared frequencies. Previous approaches using metamaterials were not successful in realizing broadband high refractive indices. A broadband high-refractive-index metamaterial structure was theoretically investigated only recently, but the proposed structure does not lend itself to easy implementation. Here we demonstrate that a broadband, extremely high index of refraction can be realized from large-area, free-standing, flexible terahertz metamaterials composed of strongly coupled unit cells. By drastically increasing the effective permittivity through strong capacitive coupling and decreasing the diamagnetic response with a thin metallic structure in the unit cell, a peak refractive index of 38.6 along with a low-frequency quasi-static value of over 20 were experimentally realized for a single-layer terahertz metamaterial, while maintaining low losses. As a natural extension of these single-layer metamaterials, we fabricated quasi-three-dimensional high-refractive-index metamaterials, and obtained a maximum bulk refractive index of 33.2 along with a value of around 8 at the quasi-static limit.
通过使用超材料来控制材料的电磁特性,超越了仅使用天然存在物质所能达到的极限,这已经成为现实。各种结构的人造“原子”的范围承诺会产生各种各样意想不到的物理现象,其中实验实现负折射率是迄今为止的主要焦点之一。将折射率扩展到高正值范围将完成可实现折射率的范围,并为变换光学提供更多的设计灵活性。除了少数半导体和绝缘体(例如硫化铅或钛酸锶)在中红外和远红外频率下具有相当高的峰值折射率之外,天然存在的透明材料具有较小的正折射率。以前使用超材料的方法在实现宽带高折射率方面并不成功。最近才理论上研究了宽带高折射率超材料结构,但所提出的结构不容易实现。在这里,我们证明了由大面积、独立式、柔性太赫兹超材料组成的宽带、极高折射率可以实现。通过在单元中采用强电容耦合大大提高有效介电常数,并通过薄金属结构降低抗磁性响应,我们在单层太赫兹超材料中实现了 38.6 的峰值折射率和低频准静态值超过 20,同时保持低损耗。作为这些单层超材料的自然扩展,我们制造了准三维高折射率超材料,并获得了最大体折射率为 33.2,准静态极限约为 8。