2022
DOI: 10.3389/fmats.2022.966535
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Active control of dual electromagnetically induced transparency in terahertz graphene-metal hybrid metasurfaces

Abstract: Active control of electromagnetically induced transparency (EIT) using metasurfaces has attracted growing interests in recent years, especially the ones that have multiple EIT windows. Here, we give out a metallic metasurface design that can achieve dual EIT (D-EIT) in the terahertz (THz) regime, and propose a strategy to individually and simultaneously control the two windows by integrating graphene structures into the design. The near-field simulations indicate that the physical mechanism lies in the composi… Show more

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Cited by 7 publications
(1 citation statement)
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“…Electromagnetic-induced transparency (EIT) is a quantum mechanical effect observed in the atomic three-energy level system due to the quantum destructive interference between two different excitation pathways, giving rise to a narrow transparency window within a broad transmission dip. This concept was then extended to plasmonic metamaterial systems. The generation of an EIT analogue in metamaterial is realized by bright-dark mode coupling and bright–bright mode coupling. The first approach requires a bright mode resonator with a low quality ( Q ) factor and a dark mode resonator with a high Q -factor. The bright mode can be directly excited by incident light, while the dark mode is activated through near-field coupling to the bright mode indirectly.…”
Section: Introductionmentioning
confidence: 99%
“…Electromagnetic-induced transparency (EIT) is a quantum mechanical effect observed in the atomic three-energy level system due to the quantum destructive interference between two different excitation pathways, giving rise to a narrow transparency window within a broad transmission dip. This concept was then extended to plasmonic metamaterial systems. The generation of an EIT analogue in metamaterial is realized by bright-dark mode coupling and bright–bright mode coupling. The first approach requires a bright mode resonator with a low quality ( Q ) factor and a dark mode resonator with a high Q -factor. The bright mode can be directly excited by incident light, while the dark mode is activated through near-field coupling to the bright mode indirectly.…”
Section: Introductionmentioning
confidence: 99%