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Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene

In this paper, a multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene is proposed, which has the advantages of polarization independence, tunability, high sensitivity, high figure of merit, etc. The device consists of a top layer dart-like patterned single-layer gra...

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Autores principales: Chen, Hao, Chen, Zihao, Yang, Hua, Wen, Lianghua, Yi, Zao, Zhou, Zigang, Dai, Bo, Zhang, Jianguo, Wu, Xianwen, Wu, Pinghui
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8982188/
https://www.ncbi.nlm.nih.gov/pubmed/35424732
http://dx.doi.org/10.1039/d2ra00611a
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author Chen, Hao
Chen, Zihao
Yang, Hua
Wen, Lianghua
Yi, Zao
Zhou, Zigang
Dai, Bo
Zhang, Jianguo
Wu, Xianwen
Wu, Pinghui
author_facet Chen, Hao
Chen, Zihao
Yang, Hua
Wen, Lianghua
Yi, Zao
Zhou, Zigang
Dai, Bo
Zhang, Jianguo
Wu, Xianwen
Wu, Pinghui
author_sort Chen, Hao
collection PubMed
description In this paper, a multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene is proposed, which has the advantages of polarization independence, tunability, high sensitivity, high figure of merit, etc. The device consists of a top layer dart-like patterned single-layer graphene array, a thicker silicon dioxide spacer layer and a metal reflector layer, and has simple structural characteristics. The numerical results show that the device achieves the perfect polarization-independent absorption at the resonance wavelengths of λ(I) = 3369.55 nm, λ(II) = 3508.35 nm, λ(III) = 3689.09 nm and λ(IV) = 4257.72 nm, with the absorption efficiencies of 99.78%, 99.40%, 99.04% and 99.91%, respectively. The absorption effect of the absorber can be effectively regulated and controlled by adjusting the numerical values such as the geometric parameters and the structural period p of the single-layer graphene array. In addition, by controlling the chemical potential and the relaxation time of the graphene layer, the resonant wavelength and the absorption efficiency of the mode can be dynamically tuned. And can keep high absorption in a wide incident angle range of 0° to 50°. At last, we exposed the structure to different environmental refractive indices, and obtained the corresponding maximum sensitivities in four resonance modes, which are S(I) = 635.75 nm RIU(−1), S(II) = 695.13 nm RIU(−1), S(III) = 775.38 nm RIU(−1) and S(IV) = 839.39 nm RIU(−1). Maximum figure of merit are 54.03 RIU(−1), 51.49 RIU(−1), 43.56 RIU(−1), and 52.14 RIU(−1), respectively. Therefore, this study has provided a new inspiration for the design of the graphene-based tunable multi-band perfect metamaterial absorber, which can be applied to the fields such as photodetectors and chemical sensors.
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spelling pubmed-89821882022-04-13 Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene Chen, Hao Chen, Zihao Yang, Hua Wen, Lianghua Yi, Zao Zhou, Zigang Dai, Bo Zhang, Jianguo Wu, Xianwen Wu, Pinghui RSC Adv Chemistry In this paper, a multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene is proposed, which has the advantages of polarization independence, tunability, high sensitivity, high figure of merit, etc. The device consists of a top layer dart-like patterned single-layer graphene array, a thicker silicon dioxide spacer layer and a metal reflector layer, and has simple structural characteristics. The numerical results show that the device achieves the perfect polarization-independent absorption at the resonance wavelengths of λ(I) = 3369.55 nm, λ(II) = 3508.35 nm, λ(III) = 3689.09 nm and λ(IV) = 4257.72 nm, with the absorption efficiencies of 99.78%, 99.40%, 99.04% and 99.91%, respectively. The absorption effect of the absorber can be effectively regulated and controlled by adjusting the numerical values such as the geometric parameters and the structural period p of the single-layer graphene array. In addition, by controlling the chemical potential and the relaxation time of the graphene layer, the resonant wavelength and the absorption efficiency of the mode can be dynamically tuned. And can keep high absorption in a wide incident angle range of 0° to 50°. At last, we exposed the structure to different environmental refractive indices, and obtained the corresponding maximum sensitivities in four resonance modes, which are S(I) = 635.75 nm RIU(−1), S(II) = 695.13 nm RIU(−1), S(III) = 775.38 nm RIU(−1) and S(IV) = 839.39 nm RIU(−1). Maximum figure of merit are 54.03 RIU(−1), 51.49 RIU(−1), 43.56 RIU(−1), and 52.14 RIU(−1), respectively. Therefore, this study has provided a new inspiration for the design of the graphene-based tunable multi-band perfect metamaterial absorber, which can be applied to the fields such as photodetectors and chemical sensors. The Royal Society of Chemistry 2022-03-09 /pmc/articles/PMC8982188/ /pubmed/35424732 http://dx.doi.org/10.1039/d2ra00611a Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Chen, Hao
Chen, Zihao
Yang, Hua
Wen, Lianghua
Yi, Zao
Zhou, Zigang
Dai, Bo
Zhang, Jianguo
Wu, Xianwen
Wu, Pinghui
Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title_full Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title_fullStr Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title_full_unstemmed Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title_short Multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
title_sort multi-mode surface plasmon resonance absorber based on dart-type single-layer graphene
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8982188/
https://www.ncbi.nlm.nih.gov/pubmed/35424732
http://dx.doi.org/10.1039/d2ra00611a
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