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基于赝表面等离激元模式的微波双折射超材料用于偏振转换。

Microwave birefringent metamaterials for polarization conversion based on spoof surface plasmon polariton modes.

机构信息

College of Science, Air Force Engineering University, Xi,an 710051, People's Republic of China.

Electronic Materials Research Laboratory, Key Laboratory of Ministry of Education, Xi'an Jiao-tong University, Xi'an 710049, People's Republic of China.

出版信息

Sci Rep. 2016 Oct 4;6:34518. doi: 10.1038/srep34518.

DOI:10.1038/srep34518
PMID:27698443
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5048301/
Abstract

We propose the design of wideband birefringent metamaterials based on spoof surface plasmon polaritons (SSPPs). Spatial k-dispersion design of SSPP modes in metamaterials is adopted to achieve high-efficiency transmission of electromagnetic waves through the metamaterial layer. By anisotropic design, the transmission phase accumulation in metamaterials can be independently modulated for x- and y-polarized components of incident waves. Since the dispersion curve of SSPPs is nonlinear, frequency-dependent phase differences can be obtained between the two orthogonal components of transmitted waves. As an example, we demonstrate a microwave birefringent metamaterials composed of fishbone structures. The full-polarization-state conversions on the zero-longitude line of Poincaré sphere can be fulfilled twice in 6-20 GHz for both linearly polarized (LP) and circularly polarized (CP) waves incidence. Besides, at a given frequency, the full-polarization-state conversion can be achieved by changing the polarization angle of the incident LP waves. Both the simulation and experiment results verify the high-efficiency polarization conversion functions of the birefringent metamaterial, including circular-to-circular, circular-to-linear(linear-to-circular), linear-to-linear polarization conversions.

摘要

我们提出了基于赝表面等离激元(SSPPs)的宽带双折射超材料的设计。采用超材料中 SSPP 模式的空间 k 色散设计来实现电磁波通过超材料层的高效传输。通过各向异性设计,可以独立调节入射波的 x 和 y 偏振分量的传输相位累积。由于 SSPP 的色散曲线是非线性的,因此可以在传输波的两个正交分量之间获得频率相关的相位差。例如,我们展示了一种由鱼骨结构组成的微波双折射超材料。在 6-20GHz 范围内,对于线偏振(LP)和圆偏振(CP)波入射,在庞加莱球的零经度线上可以实现两次全偏振态转换。此外,在给定频率下,通过改变入射 LP 波的偏振角可以实现全偏振态转换。模拟和实验结果均验证了双折射超材料的高效偏振转换功能,包括圆-圆、圆-线(线-圆)、线-线偏振转换。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/e910c18b3aff/srep34518-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/cb0ac8c87d04/srep34518-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/e2756e19f474/srep34518-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/688bd7e0c8d8/srep34518-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/7bb6e5c406de/srep34518-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/80f1cc00bfc1/srep34518-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/c99c329ba804/srep34518-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/6923c0e3b64f/srep34518-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/1eee70139b93/srep34518-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/e910c18b3aff/srep34518-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/cb0ac8c87d04/srep34518-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/e2756e19f474/srep34518-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/688bd7e0c8d8/srep34518-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/7bb6e5c406de/srep34518-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/80f1cc00bfc1/srep34518-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/c99c329ba804/srep34518-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/6923c0e3b64f/srep34518-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/1eee70139b93/srep34518-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/967a/5048301/e910c18b3aff/srep34518-f9.jpg

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