2022
DOI: 10.1364/oe.469962
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THz absorbers with an ultrahigh Q-factor empowered by the quasi-bound states in the continuum for sensing application

Abstract: The exceptional resonances excited by symmetry-protected quasi-bound states in the continuum (QBICs) have provided significant potential in high-sensitive sensing applications. Herein, we have proposed a type of metal-insulator-metal (MIM) absorbers supported by QBIC-induced resonances, and the ideal Q-factors of QBIC-induced resonances can be enhanced up to 105 in the THz regime. The coupled mode theory and the multipole scattering theory are employed to thoroughly interpret the QBIC-induced absorption mechan… Show more

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Cited by 23 publications
(9 citation statements)
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“…When the intrinsic Q-BIC is excited by the LCP light under the oblique incidence of Φ = 0°, the dynamic equations for the single-port system are described by 74 …”
Section: Simulation and Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…When the intrinsic Q-BIC is excited by the LCP light under the oblique incidence of Φ = 0°, the dynamic equations for the single-port system are described by 74 …”
Section: Simulation and Discussionmentioning
confidence: 99%
“…The γ = δ suggests that the energy is coupled into the system at the same rate as that of the dissipation, and thus is defined as the critical coupling. 74 Besides the critical coupling, the γ < δ is defined as the under coupling, whereas the γ > δ is defined as the over coupling. At the under coupling of γ < δ , the reflection coefficient at the resonant frequency ω 0 is expressed as…”
Section: Simulation and Discussionmentioning
confidence: 99%
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“…To reveal the differences in the coupling of different arrangements, we employ temporal coupled mode theory (TCMT) to fit the transmission results. The dynamical equation of the coupled system can be described as 42,43 = +…”
Section: ■ Principle and Designmentioning
confidence: 99%
“…To reveal the differences in the coupling of different arrangements, we employ temporal coupled mode theory (TCMT) to fit the transmission results. The dynamical equation of the coupled system can be described as , d a i d t = j true[ .25ex2ex lefttrue ω 1 k k ω 2 true] a i [ γ 1 γ 12 γ 21 γ 2 ] a i + true[ .25ex2ex lefttrue k 11 k 12 k 21 k 22 true] s i + where the first term on the right side of the equal sign is the Hamiltonian of the system, ω i is the resonance frequencies of the intrinsic modes, a i is the positive frequency amplitude, and k is the coupling coefficient between two modes. The second term represents the loss (γ i and γ i j = γ i γ j ), and the third term ( k ij ) is the coupling coefficient between the ports and the modes.…”
Section: Principle and Designmentioning
confidence: 99%