Hasan Md Rabiul, Hellesø Olav Gaute
Department of Physics and Technology, UiT-The Arctic University of Norway, Tromsø, Norway.
Nanotechnology. 2021 May 14;32(20):202001. doi: 10.1088/1361-6528/abdceb.
Nanophotonics allows the manipulation of light on the subwavelength scale. Optical nanoantennas are nanoscale elements that enable increased resolution in bioimaging, novel photon sources, solar cells with higher absorption, and the detection of fluorescence from a single molecule. While plasmonic nanoantennas have been extensively explored in the literature, dielectric nanoantennas have several advantages over their plasmonic counterparts, including low dissipative losses and near-field enhancement of both electric and magnetic fields. Nanoantennas increase the optical density of states, which increase the rate of spontaneous emission due to the Purcell effect. The increase is quantified by the Purcell factor, which depends on the mode volume and the quality factor. It is one of the main performance parameters for nanoantennas. One particularly interesting feature of dielectric nanoantennas is the possibility of integrating them into optical resonators with a high quality-factor, further improving the performance of the nanoantennas and giving very high Purcell factors. This review introduces the properties and parameters of dielectric optical nanoantennas, and gives a classification of the nanoantennas based on the number and shape of the nanoantenna elements. An overview of recent progress in the field is provided, and a simulation is included as an example. The simulated nanoantenna, a dimer consisting of two silicon nanospheres separated by a gap, is shown to have a very small mode volume, but a low quality-factor. Some recent works on photonic crystal resonators are reviewed, including one that includes a nanoantenna in the bowtie unit-cell. This results in an enormous increase in the calculated Purcell factor, from 200 for the example dimer, to 8 × 10 for the photonic crystal resonator. Some applications of dielectric nanoantennas are described. With current progress in the field, it is expected that the number of applications will grow and that nanoantennas will be incorporated into new commercial products. A list of relevant materials with high refractive indexes and low losses is presented and discussed. Finally, prospects and major challenges for dielectric nanoantennas are addressed.
纳米光子学能够在亚波长尺度上对光进行操控。光学纳米天线是纳米级元件,可实现生物成像中更高的分辨率、新型光子源、具有更高吸收率的太阳能电池以及单分子荧光检测。虽然等离激元纳米天线在文献中已得到广泛研究,但介电纳米天线相较于其等离激元同类具有若干优势,包括低耗散损耗以及电场和磁场的近场增强。纳米天线增加了态密度,由于珀塞尔效应,这会提高自发发射速率。这种增加由珀塞尔因子量化,珀塞尔因子取决于模式体积和品质因数。它是纳米天线的主要性能参数之一。介电纳米天线一个特别有趣的特性是有可能将它们集成到具有高品质因数的光学谐振器中,进一步提高纳米天线的性能并给出非常高的珀塞尔因子。本综述介绍了介电光学纳米天线的特性和参数,并根据纳米天线元件的数量和形状对纳米天线进行了分类。提供了该领域近期进展的概述,并包含一个模拟示例。所模拟的纳米天线是由两个被间隙隔开的硅纳米球组成的二聚体,显示出非常小的模式体积,但品质因数较低。综述了近期关于光子晶体谐振器的一些工作,包括在领结晶胞中包含纳米天线的一项工作。这导致计算出的珀塞尔因子大幅增加,从示例二聚体的200增加到光子晶体谐振器的8×10⁴。描述了介电纳米天线的一些应用。随着该领域目前的进展,预计应用数量将会增加,并且纳米天线将被纳入新的商业产品中。列出并讨论了具有高折射率和低损耗的相关材料清单。最后,探讨了介电纳米天线的前景和主要挑战。