Abstract:Bound states in the continuum (BIC) is an exotic concept describing systems without radiative loss. BICs are widely investigated in optics due to numerous potential applications including lasing, sensing, and filtering, among others. This study introduces a structurally tunable BIC terahertz metamaterial fabricated using micromachining and experimentally characterized using terahertz time domain spectroscopy. Control of the bending angle of the metamaterial by thermal actuation modifies the capacitance enablin… Show more
“…In the numerical calculations, the basic size parameters of the unit cell are optimized by the CST and determined as follows: P = 26 µm; l 1 = 18 µm; l 2 = 15.17 µm; w = 2 µm; α = 45 • ; β = 22.5 • ; h 1 = 0.2 µm; h 2 = 10 µm; and h 3 = 2 µm. The gold film with a conductivity of 4.56 × 10 7 S/m is patterned to create the Z-shaped anisotropic metal structures [29], and the lossless polyimide with the permittivity of εPI = 3.5 is selected as the dielectric layer material [30].…”
Section: Design and Simulation Of Metasurface Unit Cellsmentioning
Currently, vortex beams are extensively utilized in the information transmission and storage of communication systems due to their additional degree of freedom. However, traditional terahertz metasurfaces only focus on the generation of narrowband vortex beams in reflection or transmission mode, which is unbeneficial for practical applications. Here, we propose and design terahertz metasurface unit cells composed of anisotropic Z-shaped metal structures, two dielectric layers, and a VO2 film layer. By utilizing the Pancharatnam–Berry phase theory, independent control of a full 2π phase over a wide frequency range can be achieved by rotating the unit cell. Moreover, the full-space mode (transmission and reflection) can also be implemented by utilizing the phase transition of VO2 film. Based on the convolution operation, three different terahertz metasurfaces are created to generate vortex beams with different wavefronts in full-space, such as deflected vortex beams, focused vortex beams, and non-diffraction vortex beams. Additionally, the divergences of these vortex beams are also analyzed. Therefore, our designed metasurfaces are capable of efficiently shaping the wavefronts of broadband vortex beams in full-space, making them promising applications for long-distance transmission, high integration, and large capacity in 6G terahertz communications.
“…In the numerical calculations, the basic size parameters of the unit cell are optimized by the CST and determined as follows: P = 26 µm; l 1 = 18 µm; l 2 = 15.17 µm; w = 2 µm; α = 45 • ; β = 22.5 • ; h 1 = 0.2 µm; h 2 = 10 µm; and h 3 = 2 µm. The gold film with a conductivity of 4.56 × 10 7 S/m is patterned to create the Z-shaped anisotropic metal structures [29], and the lossless polyimide with the permittivity of εPI = 3.5 is selected as the dielectric layer material [30].…”
Section: Design and Simulation Of Metasurface Unit Cellsmentioning
Currently, vortex beams are extensively utilized in the information transmission and storage of communication systems due to their additional degree of freedom. However, traditional terahertz metasurfaces only focus on the generation of narrowband vortex beams in reflection or transmission mode, which is unbeneficial for practical applications. Here, we propose and design terahertz metasurface unit cells composed of anisotropic Z-shaped metal structures, two dielectric layers, and a VO2 film layer. By utilizing the Pancharatnam–Berry phase theory, independent control of a full 2π phase over a wide frequency range can be achieved by rotating the unit cell. Moreover, the full-space mode (transmission and reflection) can also be implemented by utilizing the phase transition of VO2 film. Based on the convolution operation, three different terahertz metasurfaces are created to generate vortex beams with different wavefronts in full-space, such as deflected vortex beams, focused vortex beams, and non-diffraction vortex beams. Additionally, the divergences of these vortex beams are also analyzed. Therefore, our designed metasurfaces are capable of efficiently shaping the wavefronts of broadband vortex beams in full-space, making them promising applications for long-distance transmission, high integration, and large capacity in 6G terahertz communications.
“…Usually, quasi-BIC can be stimulated in geometry symmetry-broken, oblique incidence, or coupling-mode resonant system, respectively, named as symmetry-protected BIC [26,27] and accidental BIC, [28] and shows considerable sensitivity and tunability in both geometry parameter space and incident momentum space. [29][30][31] From the first experiment observation of quasi-BIC in photonic crystal (PhC) in 2013, [32] periodic micro-nano structures such as PhCs and metamaterials have been an ideal platform to deeply research and practically apply quasi-BIC owing to their highly artificial designability and complementary metal-oxide-semiconductor compatibility in wide spectra ranging from terahertz to visible spectra. [33] In 2018, Koshelev et al proposed a series of in-plane asymmetry resonator designs using high-refractive-index dielectrics or metals and demonstrated their quasi-BIC properties.…”
Quasibound states in the continuum (BIC) have earned extensive attentions due to the capability to realize extremely high quality‐factor (Q‐factor) resonance. Here, a metamaterial composed of silicon dioxide (SiO2) with low refractive index (≈1.45) on gold (Au) reflection mirror is proposed to realize narrowband perfect absorption with the assistance of quasi‐BIC and surface lattice resonance. The proposed SiO2‐Au absorber based on SiO2 metamaterial is composed of two tilted SiO2 cubes into a unit cell and periodically arranged on Au reflection mirror. By optimizing the geometry parameters, the proposed absorber presents both accidental quasi‐BIC and symmetry‐protected quasi‐BIC modes with near‐perfect absorptivity and high Q‐factor of 2330 and 1438, respectively. The Q‐factor can be further improved to 104 by increasing the thickness of SiO2 cubes to micrometer level. Meanwhile, the wavelength of absorption peak shows linear sensitivity of 16.67 and 17.88 nm per degree to incident angles as the absorptivity is higher than 92% and 75% in the spectra range of 215.0–141.0 nm, respectively. These results open the avenue for the metamaterial absorber in emitter, imaging, and biosensing applications.
The remarkable properties of toroidal metasurfaces, featuring ultrahigh‐Q bound states in the continuum (BIC) resonances and nonradiating anapole modes, have garnered significant attention. The active manipulation of quasi‐BIC resonance characteristics offers substantial potential for advancing tunable metasurfaces. This study explores explicitly the application of vanadium dioxide, a phase change material widely used in active photonics and room‐temperature bolometric detectors, to control quasi‐BIC resonances in toroidal metasurfaces. The phase change transition of vanadium dioxide occurs in a narrow temperature range, providing a large variation in material resistivity. Through heating thin film patches of vanadium dioxide integrated into a metasurface comprising gold split‐ring resonators on a sapphire substrate, remarkable control over the amplitude and frequency of quasi‐BIC resonances is achieved due to their high sensitivity to losses present in the system. Breaking the symmetry of meta‐atoms reveals enhanced tunability. The predicted maximum change in the quasi‐BIC resonance amplitude reaches 14 dB with a temperature variation of ≈10 °C.
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