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基于复合石墨烯和二氧化钒超材料的双比特双频可切换太赫兹吸收器。

Two bits dual-band switchable terahertz absorber enabled by composite graphene and vanadium dioxide metamaterials.

作者信息

Barzegar-Parizi Saeedeh, Ebrahimi Amir, Ghorbani Kamran

机构信息

Electrical Engineering Department, Sirjan University of Technology, Sirjan, Iran.

School of Engineering, RMIT University, Melbourne, Australia.

出版信息

Sci Rep. 2024 Mar 9;14(1):5818. doi: 10.1038/s41598-024-56349-y.

DOI:10.1038/s41598-024-56349-y
PMID:38461328
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10924928/
Abstract

This article presents the design of a 2-bit dual-band switchable terahertz absorber using a stacked combination of graphene and vanadium dioxide (VO) metamaterials. For the first time, the proposed absorber design offers four switchable states by controlling the conductivity of graphene and VO metamaterial layers. The lower absorption band is produced by the graphene metamaterial, whereas the upper band is implemented by the VO metamaterial pattern. The structure shows two absorption bands (State 11) at 0.745-0.775 THz and 2.3-5.63 THz, when the Fermi graphene level of graphene is 0.2 eV and the VO is in the metallic phase. The lower absorption band is turned off, while keeping the upper band (State 01), when the graphene Fermi level is 0 eV and the VO layer is in the metallic phase. The upper absorption band is turned off, while preserving the lower absorption band (State 10) by switching the VO into the insulator phase and keeping the graphene Fermi level at 0.2 eV. Finally, both of the absorption bands are turned off by setting the graphene Fermi level to 0 eV and switching the VO into the insulating phase. Equivalent circuit modelling analysis and full-wave electromagnetic simulations are used to explain the operation principle of the proposed absorber. Very good agreement is obtained between the theoretical analysis and the simulations confirming the presented design principle for the 2-bit switchable absorber.

摘要

本文介绍了一种采用石墨烯和二氧化钒(VO)超材料堆叠组合设计的2比特双波段可切换太赫兹吸收器。该吸收器设计首次通过控制石墨烯和VO超材料层的电导率提供了四种可切换状态。较低的吸收带由石墨烯超材料产生,而较高的吸收带则由VO超材料图案实现。当石墨烯的费米能级为0.2 eV且VO处于金属相时,该结构在0.745 - 0.775 THz和2.3 - 5.63 THz处显示出两个吸收带(状态11)。当石墨烯费米能级为0 eV且VO层处于金属相时,较低的吸收带关闭,而较高的吸收带保持(状态01)。通过将VO切换到绝缘相并将石墨烯费米能级保持在0.2 eV,较高的吸收带关闭,同时保留较低的吸收带(状态10)。最后,通过将石墨烯费米能级设置为0 eV并将VO切换到绝缘相,两个吸收带都关闭。等效电路建模分析和全波电磁模拟用于解释所提出吸收器的工作原理。理论分析和模拟之间取得了很好的一致性,证实了所提出的2比特可切换吸收器的设计原理。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/e475a333746a/41598_2024_56349_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/1014b0d83e8d/41598_2024_56349_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/2f2be8436611/41598_2024_56349_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/60d07a8b056a/41598_2024_56349_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/1cf9d605c9e9/41598_2024_56349_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/81fb58f9cdaa/41598_2024_56349_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/f03239b37eb2/41598_2024_56349_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/e41c16fa9bc7/41598_2024_56349_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/e475a333746a/41598_2024_56349_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/1014b0d83e8d/41598_2024_56349_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/2f2be8436611/41598_2024_56349_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/60d07a8b056a/41598_2024_56349_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/1cf9d605c9e9/41598_2024_56349_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/81fb58f9cdaa/41598_2024_56349_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/f03239b37eb2/41598_2024_56349_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/e41c16fa9bc7/41598_2024_56349_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/cf04/10924928/e475a333746a/41598_2024_56349_Fig8_HTML.jpg

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