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超宽带偏振无关纳米结构：用于可见光和红外光学窗口应用的完美超材料吸收体

Ultrawideband Polarization-Independent Nanoarchitectonics: A Perfect Metamaterial Absorber for Visible and Infrared Optical Window Applications.

作者信息

Hakim Mohammad Lutful, Hanif Abu, Alam Touhidul, Islam Mohammad Tariqul, Arshad Haslina, Soliman Mohamed S, Albadran Saleh Mohammad, Islam Md Shabiul

机构信息

Pusat Sains Ankasa (ANGKASA), Institut Perubahan Iklim, Universiti Kebangsaan Malaysia (UKM), Bangi 43600, Selangor, Malaysia.

Department of CSE, International Islamic University Chittagong (IIUC), Kumira, Chattogram 4318, Bangladesh.

出版信息

Nanomaterials (Basel). 2022 Aug 18;12(16):2849. doi: 10.3390/nano12162849.

DOI:10.3390/nano12162849
PMID:36014711
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9412529/
Abstract

This article presents numerical analysis of an ultrathin concentric hexagonal ring resonator (CHRR) metamaterial absorber (MMA) for ultrawideband visible and infrared optical window applications. The proposed MMA exhibits an absorption of above 90% from 380 to 2500 nm and an average absorbance of 96.64% at entire operational bandwidth with a compact unit cell size of 66 × 66 nm. The designed MMA shows maximum absorption of 99% at 618 nm. The absorption bandwidth of the MMA covers the entire visible and infrared optical windows. The nickel material has been used to design the top and bottom layer of MMA, where aluminium nitride (AlN) has been used as the substrate. The designed hexagonal MMA shows polarization-independent properties due to the symmetry of the design and a stable absorption label is also achieved for oblique incident angles up to 70 °C. The absorption property of hexagonal ring resonator MMA has been analyzed by design evaluation, parametric and various material investigations. The metamaterial property, surface current allocation, magnetic field and electric field have also been analyzed to explore the absorption properties. The proposed MMA has promising prospects in numerous applications like infrared detection, solar cells, gas detection sensors, imaging, etc.

摘要

本文介绍了一种用于超宽带可见光和红外光学窗口应用的超薄同心六边形环谐振器（CHRR）超材料吸收体（MMA）的数值分析。所提出的MMA在380至2500 nm范围内表现出高于90%的吸收率，在整个工作带宽内平均吸收率为96.64%，单元尺寸紧凑，为66×66 nm。设计的MMA在618 nm处显示出99%的最大吸收率。MMA的吸收带宽覆盖了整个可见光和红外光学窗口。镍材料用于设计MMA的顶层和底层，其中氮化铝（AlN）用作衬底。由于设计的对称性，所设计的六边形MMA显示出与偏振无关的特性，并且对于高达70°C的斜入射角也实现了稳定的吸收标记。通过设计评估、参数分析和各种材料研究，分析了六边形环谐振器MMA的吸收特性。还分析了超材料特性、表面电流分布、磁场和电场，以探索吸收特性。所提出的MMA在红外探测、太阳能电池、气体检测传感器、成像等众多应用中具有广阔的前景。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/098795785cf6/nanomaterials-12-02849-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/e4be8f883654/nanomaterials-12-02849-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/43b75dbfe3b3/nanomaterials-12-02849-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/11c5b2d29ca2/nanomaterials-12-02849-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/a3a45b530a10/nanomaterials-12-02849-g004a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/5724034dd3d5/nanomaterials-12-02849-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/f15d2f7b18f5/nanomaterials-12-02849-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/ae9d10a3f33f/nanomaterials-12-02849-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/24963c17a03b/nanomaterials-12-02849-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/6b006a0d5e02/nanomaterials-12-02849-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/bcee2054baff/nanomaterials-12-02849-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/7e8c84eb2388/nanomaterials-12-02849-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/71521d239369/nanomaterials-12-02849-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/0623be1e09a4/nanomaterials-12-02849-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/098795785cf6/nanomaterials-12-02849-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/e4be8f883654/nanomaterials-12-02849-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/43b75dbfe3b3/nanomaterials-12-02849-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/11c5b2d29ca2/nanomaterials-12-02849-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/a3a45b530a10/nanomaterials-12-02849-g004a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/5724034dd3d5/nanomaterials-12-02849-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/f15d2f7b18f5/nanomaterials-12-02849-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/ae9d10a3f33f/nanomaterials-12-02849-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/24963c17a03b/nanomaterials-12-02849-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/6b006a0d5e02/nanomaterials-12-02849-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/bcee2054baff/nanomaterials-12-02849-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/7e8c84eb2388/nanomaterials-12-02849-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/71521d239369/nanomaterials-12-02849-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/0623be1e09a4/nanomaterials-12-02849-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f161/9412529/098795785cf6/nanomaterials-12-02849-g014.jpg

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