材料稀疏结构中的导模共振纳米光子学

SPIE OPTO Pub Date : 2016-03-15 DOI:10.1117/12.2211687
R. Magnusson, Manoj Niraula, J. Yoon, Y. Ko, K. Lee
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引用次数: 4

摘要

导模共振(GMR)的概念是指在周期层中诱导的横向准导波导模式。尽管这些影响早已为人所知,但新的属性和创新仍在不断出现。在这里,我们回顾了该领域的一些最新进展,重点是稀疏或最小的设备实施例。我们讨论了用光栅设计的宽带谐振反射器的特性,其中光栅脊与相同的材料匹配以消除局部反射和相位变化。因此,这个临界界面具有零折射率对比度;因此我们称它们为“零对比度光栅”。应用这种结构,我们提出了在实验实际参数变化下具有鲁棒性的单层宽带反射器。我们介绍了一种新型的反射器和偏振器,这种反射器和偏振器由介质纳米线网格构成,这些网格大部分是空的。计算结果预测了这些稀疏晶格的高反射和伴随的偏振消光。用硅纳米线网格进行实验验证,得到了单偏振态~200 nm宽的高反射带和正交态的自由透射。最后,我们提出了采用全介电谐振光栅的带通滤波器。我们设计,制造和测试了具有高效率和亚纳米宽通带的纳米结构单层滤波器,并被100纳米宽的阻带包围。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Guided-mode resonance nanophotonics in materially sparse architectures
The guided-mode resonance (GMR) concept refers to lateral quasi-guided waveguide modes induced in periodic layers. Whereas these effects have been known for a long time, new attributes and innovations continue to appear. Here, we review some recent progress in this field with emphasis on sparse, or minimal, device embodiments. We discuss properties of wideband resonant reflectors designed with gratings in which the grating ridges are matched to an identical material to eliminate local reflections and phase changes. This critical interface therefore possesses zero refractive-index contrast; hence we call them “zero-contrast gratings.” Applying this architecture, we present single-layer, wideband reflectors that are robust under experimentally realistic parametric variations. We introduce a new class of reflectors and polarizers fashioned with dielectric nanowire grids that are mostly empty space. Computed results predict high reflection and attendant polarization extinction for these sparse lattices. Experimental verification with Si nanowire grids yields ~200-nm-wide band of high reflection for one polarization state and free transmission of the orthogonal state. Finally, we present bandpass filters using all-dielectric resonant gratings. We design, fabricate, and test nanostructured single layer filters exhibiting high efficiency and sub-nanometer-wide passbands surrounded by 100-nm-wide stopbands.
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