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Thematische Bibliographien / MULTIBAND METAMATERIAL ABSORBER (MMA)

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Auswahl der wissenschaftlichen Literatur zum Thema „MULTIBAND METAMATERIAL ABSORBER (MMA)“

Autor: Grafiati

Veröffentlicht am 26. Oktober 2023

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Zeitschriftenartikel zum Thema "MULTIBAND METAMATERIAL ABSORBER (MMA)"

1

Mohanty, Ayesha, Om Prakash Acharya, Bhargav Appasani, Kriangkrai Sooksood, and Sushanta Kumar Mohapatra. "A THz Metamaterial Absorber with Multiple Polarization - Insensitive, Sensitive, and Tunable." ECTI Transactions on Electrical Engineering, Electronics, and Communications 19, no. 2 (2021): 165–73. http://dx.doi.org/10.37936/ecti-eec.2021192.242019.

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Terahertz (THz) absorbers are gaining interest in many applications. In this paper, we present the design and simulation of a multiband metamaterial absorber (MMA) with combined polarization properties and prominent absorption at 2.2 THz and 3.9 THz. The MMA comprises two square split-ring resonators and one square ring resonator placed on top of a polyimide dielectric spacer, offering multiband absorption characteristics with maximum absorptivity of 93.18% and 96.09%, respectively. The most protruding feature of this design is that it displays multiple polarization characteristics, including

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2

Saxena, G., Y. Khanna, Y. K. Awasthi, and P. Jain. "Multi-Band Polarization Insensitive Ultra-Thin THz Metamaterial Absorber for Imaging and EMI Shielding Applications." Advanced Electromagnetics 10, no. 3 (2021): 43–49. http://dx.doi.org/10.7716/aem.v10i3.1759.

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this article, a multi-band polarization-insensitive metamaterial absorber is designed for THz imaging and EMI shielding. A unique oval-shaped structure with three circular ring-shaped resonators is proposed with a unit cell dimension of36×36×19.6μm3. The absorbance of the proposed multiband MMA is 98.57%, 90%and 99.85% at 5.58, 7.98-8.84, 11.45THz frequency respectively. Return loss is nearly the same for the changing incident and polarization angle. Therefore, this metamaterial absorber with a wide range of polarization insensitivity is found and it is also suitable for quantum RADAR Imaging,

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3

Hakim, Mohammad Lutful, Touhidul Alam, Mohammad Tariqul Islam, Mohd Hafiz Baharuddin, Ahmed Alzamil, and Md Shabiul Islam. "Quad-Band Polarization-Insensitive Square Split-Ring Resonator (SSRR) with an Inner Jerusalem Cross Metamaterial Absorber for Ku- and K-Band Sensing Applications." Sensors 22, no. 12 (2022): 4489. http://dx.doi.org/10.3390/s22124489.

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The development of metamaterial absorbers has become attractive for various fields of application, such as sensing, detectors, wireless communication, antenna design, emitters, spatial light modulators, etc. Multiband absorbers with polarization insensitivity have drawn significant attention in microwave absorption and sensing research. In this paper, we propose a quad-band polarization-insensitive metamaterial absorber (MMA) for Ku- and K-band applications. The proposed patch comprises two square split-ring resonators (SSRR), four microstrip lines, and an inner Jerusalem cross to generate fou

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4

Wang, Wenjie, Mingde Feng, Jun Wang, et al. "Quadruple-band metamaterial absorber based on the cuboid dielectric particles." Journal of Advanced Dielectrics 08, no. 04 (2018): 1850023. http://dx.doi.org/10.1142/s2010135x18500236.

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In this work, a quadruple-band dielectric metamaterial absorber (MMA) was proposed and studied, which is composed of eight cuboid dielectric particles and a metallic ground plate. When electromagnetic wave is incident on the dielectric particles, dielectric particles act as resonators and produce abundant resonant modes, which can result in perfect absorption. In simulation, four absorption peaks are observed at 9.13, 9.62, 10.0 and 10.46[Formula: see text]GHz with 88%, 89%, 100% and 96%, respectively. By adjusting geometry parameters of the dielectric particles, dielectric MMAs with different

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5

Hossain, I., M. Samsuzzaman, M. S. J. Singh, B. B. Bais, and M. T. Islam. "Numerical investigation of polarization-insensitive multiband metamaterial for terahertz solar absorber." Digest Journal of Nanomaterials and Biostructures 16, no. 2 (2021): 593–600. http://dx.doi.org/10.15251/djnb.2021.162.593.

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This study presents a nanostructured multiband metamaterial absorber for the optical regime application. The proposed structure is exhibited 0° to 90° polarization insensitivity and up to 45° angular stability with more than 90% peak absorption in between 300 THz800 THz frequency range. Proposed MMA structure is acquired perfect absorption of 99.99% at 571THz, 99.50% at 488.26 THz, 99.32% at 598 THz frequency by adjusting geometrical parameters. Due to perfect impedance matching with plasmonic resonance characteristics, these structures achieved an average absorption of 95.30%, 91.96%, 97.25%,

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6

Wu, Han, Shijun Ji, Ji Zhao, Chengxin Jiang, and Handa Dai. "Design and Analysis of a Five-Band Polarization-Insensitive Metamaterial Absorber." International Journal of Antennas and Propagation 2020 (December 7, 2020): 1–12. http://dx.doi.org/10.1155/2020/8827517.

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A five-band metamaterial absorber (MMA) is presented. The proposed absorber consists of a three-layer structure of the top metal resonator, intermediate dielectric layer, and bottom metal plane. The top structure takes the centroid as the center and spreads out in a three-pronged shape with an average of 360°, and the ends bifurcate again. The calculation was carried out by the professional software to iteratively optimize the absorption effect of MMA in the microwave range. The results show that the MA has five peaks at resonant frequencies of 5.984 GHz, 12.232 GHz, 18.128 GHz, 18.414 GHz, an

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7

Hannan, Islam, Hoque, Singh, and Almutairi. "Design of a Novel Double Negative Metamaterial Absorber Atom for Ku and K Band Applications." Electronics 8, no. 8 (2019): 853. http://dx.doi.org/10.3390/electronics8080853.

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This paper presents a multiband metamaterial (MM) absorber based on a novel spiral resonator with continuous, dual, and opposite P-shape. The full wave analysis shows 80.06% to 99.95% absorption at frequencies range for Ku and K bands for several substrate materials of 100 mm2 area. The results indicate that the absorption rate remains similar for different polarizing angles in TEM mode with different substrates. With FR4 (Flame Retardant 4) substrate and 64 mm2 ground plane, the design acts as single negative (SNG) MM absorber in K band resonance frequencies (19.75–21.37 GHz) and acts as doub

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8

Gu, Chao, Shao-Bo Qu, Zhi-Bin Pei, Zhuo Xu, Jia Liu, and Wei Gu. "Multiband terahertz metamaterial absorber." Chinese Physics B 20, no. 1 (2011): 017801. http://dx.doi.org/10.1088/1674-1056/20/1/017801.

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9

Xu, Zong-Cheng, Run-Mei Gao, Chun-Feng Ding, Ya-Ting Zhang, and Jian-Quan Yao. "Multiband Metamaterial Absorber at Terahertz Frequencies." Chinese Physics Letters 31, no. 5 (2014): 054205. http://dx.doi.org/10.1088/0256-307x/31/5/054205.

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10

Tian, Yiran, Guangjun Wen, and Yongjun Huang. "Multiband Negative Permittivity Metamaterials and Absorbers." Advances in OptoElectronics 2013 (July 28, 2013): 1–7. http://dx.doi.org/10.1155/2013/269170.

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Design and characteristics of multiband negative permittivity metamaterial and its absorber configuration are presented in this paper. The proposed multiband metamaterial is composed of a novel multibranch resonator which can possess four electric resonance frequencies. It is shown that, by controlling the length of the main branches of such resonator, the resonant frequencies and corresponding absorbing bands of metamaterial absorber can be shifted in a large frequency band.

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