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Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene

This paper introduces a novel metamaterial absorber based on surface plasmon resonance (SPR). The absorber is capable of triple-mode perfect absorption, polarization independence, incident angle insensitivity, tunability, high sensitivity, and a high figure of merit (FOM). The structure of the absor...

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Autores principales: Lai, Runing, Shi, Pengcheng, Yi, Zao, Li, Hailiang, Yi, Yougen
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10221595/
https://www.ncbi.nlm.nih.gov/pubmed/37241576
http://dx.doi.org/10.3390/mi14050953
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author Lai, Runing
Shi, Pengcheng
Yi, Zao
Li, Hailiang
Yi, Yougen
author_facet Lai, Runing
Shi, Pengcheng
Yi, Zao
Li, Hailiang
Yi, Yougen
author_sort Lai, Runing
collection PubMed
description This paper introduces a novel metamaterial absorber based on surface plasmon resonance (SPR). The absorber is capable of triple-mode perfect absorption, polarization independence, incident angle insensitivity, tunability, high sensitivity, and a high figure of merit (FOM). The structure of the absorber consists of a sandwiched stack: a top layer of single-layer graphene array with an open-ended prohibited sign type (OPST) pattern, a middle layer of thicker SiO(2), and a bottom layer of the gold metal mirror (Au). The simulation of COMSOL software suggests it achieves perfect absorption at frequencies of f(I) = 4.04 THz, f(II) = 6.76 THz, and f(III) = 9.40 THz, with absorption peaks of 99.404%, 99.353%, and 99.146%, respectively. These three resonant frequencies and corresponding absorption rates can be regulated by controlling the patterned graphene’s geometric parameters or just adjusting the Fermi level (E(F)). Additionally, when the incident angle changes between 0~50°, the absorption peaks still reach 99% regardless of the kind of polarization. Finally, to test its refractive index sensing performance, this paper calculates the results of the structure under different environments which demonstrate maximum sensitivities in three modes: S(I) = 0.875 THz/RIU, S(II) = 1.250 THz/RIU, and S(III) = 2.000 THz/RIU. The FOM can reach FOM(I) = 3.74 RIU(−1), FOM(II) = 6.08 RIU(−1), and FOM(III) = 9.58 RIU(−1). In conclusion, we provide a new approach for designing a tunable multi-band SPR metamaterial absorber with potential applications in photodetectors, active optoelectronic devices, and chemical sensors.
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spelling pubmed-102215952023-05-28 Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene Lai, Runing Shi, Pengcheng Yi, Zao Li, Hailiang Yi, Yougen Micromachines (Basel) Article This paper introduces a novel metamaterial absorber based on surface plasmon resonance (SPR). The absorber is capable of triple-mode perfect absorption, polarization independence, incident angle insensitivity, tunability, high sensitivity, and a high figure of merit (FOM). The structure of the absorber consists of a sandwiched stack: a top layer of single-layer graphene array with an open-ended prohibited sign type (OPST) pattern, a middle layer of thicker SiO(2), and a bottom layer of the gold metal mirror (Au). The simulation of COMSOL software suggests it achieves perfect absorption at frequencies of f(I) = 4.04 THz, f(II) = 6.76 THz, and f(III) = 9.40 THz, with absorption peaks of 99.404%, 99.353%, and 99.146%, respectively. These three resonant frequencies and corresponding absorption rates can be regulated by controlling the patterned graphene’s geometric parameters or just adjusting the Fermi level (E(F)). Additionally, when the incident angle changes between 0~50°, the absorption peaks still reach 99% regardless of the kind of polarization. Finally, to test its refractive index sensing performance, this paper calculates the results of the structure under different environments which demonstrate maximum sensitivities in three modes: S(I) = 0.875 THz/RIU, S(II) = 1.250 THz/RIU, and S(III) = 2.000 THz/RIU. The FOM can reach FOM(I) = 3.74 RIU(−1), FOM(II) = 6.08 RIU(−1), and FOM(III) = 9.58 RIU(−1). In conclusion, we provide a new approach for designing a tunable multi-band SPR metamaterial absorber with potential applications in photodetectors, active optoelectronic devices, and chemical sensors. MDPI 2023-04-27 /pmc/articles/PMC10221595/ /pubmed/37241576 http://dx.doi.org/10.3390/mi14050953 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Lai, Runing
Shi, Pengcheng
Yi, Zao
Li, Hailiang
Yi, Yougen
Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title_full Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title_fullStr Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title_full_unstemmed Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title_short Triple-Band Surface Plasmon Resonance Metamaterial Absorber Based on Open-Ended Prohibited Sign Type Monolayer Graphene
title_sort triple-band surface plasmon resonance metamaterial absorber based on open-ended prohibited sign type monolayer graphene
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10221595/
https://www.ncbi.nlm.nih.gov/pubmed/37241576
http://dx.doi.org/10.3390/mi14050953
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