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微波频段中薄腔阵列的偏振转换

Polarization conversion from a thin cavity array in the microwave regime.

作者信息

Tremain B, Rance H J, Hibbins A P, Sambles J R

机构信息

Electromagnetic and Acoustic Materials Group, Department of Physics and Astronomy, University of Exeter, Exeter. EX4 4QL, United Kingdom.

出版信息

Sci Rep. 2015 Mar 23;5:9366. doi: 10.1038/srep09366.

DOI:10.1038/srep09366
PMID:25797210
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4369744/
Abstract

Linearly polarized microwave radiation is shown to have its plane of polarization converted to the orthogonal state upon reflection from an ultrathin (λ/25) cavity array. The structure benefits from an uncomplicated design consisting of a metallic grating closely separated from a ground plane by a dielectric spacer. A single set of periodically spaced slits (monograting) exhibits polarization conversion when the normally incident electric field is aligned at 45° to the slits. Two orthogonal sets of slits (bigrating) allows this narrow-band effect to be broadened when the two orthogonal resonances are separated in frequency. We optimise the design and experimentally demonstrate near loss-less polarization conversion (95% of the incident intensity) across a 3.1 GHz frequency band. Finally, we study the dependence of the structure's performance on incident angle and slit width.

摘要

线性极化微波辐射在从超薄(λ/25)腔阵列反射时,其极化平面会转换为正交状态。该结构得益于一种简单的设计,它由一个通过介电间隔层与接地平面紧密分离的金属光栅组成。当垂直入射电场与狭缝呈45°排列时,单组周期性间隔的狭缝(单光栅)会表现出极化转换。当两个正交共振在频率上分离时,两组正交的狭缝(双光栅)能使这种窄带效应得到拓宽。我们优化了设计,并通过实验证明在3.1 GHz频带上实现了近乎无损耗的极化转换(入射强度的95%)。最后,我们研究了该结构的性能对入射角和狭缝宽度的依赖性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/e967c4555ae9/srep09366-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/673eb4741fc3/srep09366-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/d718820f654b/srep09366-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/9d8278660178/srep09366-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/1ae6d163d82d/srep09366-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/430c637e8a39/srep09366-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/f17e49af5d52/srep09366-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/88ebf0319510/srep09366-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/e967c4555ae9/srep09366-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/673eb4741fc3/srep09366-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/d718820f654b/srep09366-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/9d8278660178/srep09366-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/1ae6d163d82d/srep09366-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/430c637e8a39/srep09366-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/f17e49af5d52/srep09366-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/88ebf0319510/srep09366-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6c71/4369744/e967c4555ae9/srep09366-f8.jpg

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