Showing posts with label all-dielectric metasurface. Show all posts
Showing posts with label all-dielectric metasurface. Show all posts

Friday, October 11, 2019

Abstract-Guided‐Mode Resonances in All‐Dielectric Terahertz Metasurfaces


Song Han,  Mikhail V. Rybin, Prakash Pitchappa,  Yogesh Kumar Srivastava,  Yuri S. Kivshar,  Ranjan Singh,
Low‐loss silicon cuboid based all‐dielectric terahertz metasurfaces act simultaneously as diffraction grating and in‐plane slab waveguide, thereby enabling excitation of guided mode resonances (GMRs). At normal incidence, destructive interference between counter‐propagating GMRs give rise to symmetry‐protected bound state in the continuum. Terahertz GMRs are multifunctional devices that can enable narrow‐band filters, ultrafast modulators, and free‐space couplers.
https://onlinelibrary.wiley.com/doi/10.1002/adom.201900959

Coupling of diffracted waves in gratings with the waveguide modes gives rise to the guided mode resonances (GMRs). The GMRs provide designer linewidth and resonance intensity amidst a broad background, and thus have been widely used for numerous applications in visible and infrared spectral regions. Here, terahertz GMRs are demonstrated in low‐loss, all‐dielectric metasurfaces, which are periodic square lattices of silicon cuboids on quartz substrates. The silicon cuboid lattice simultaneously acts as a diffraction grating and an in‐plane slab waveguide, thereby resulting in the formation of terahertz GMRs. At oblique incidence, two distinct frequency detuned GMRs are observed. The frequency difference between these two GMRs increases at larger angle of incidence. However, extremely small angle of incidence causes destructive interference between these counter‐propagating GMRs that leads to a nonradiative symmetry‐protected bound state in the continuum. GMRs in all‐dielectric silicon metasurfaces can have potential applications in the realization of efficient terahertz devices such as high‐Q transmission filters with angular spectral selectivity, ultrafast modulators, and free‐space couplers.

Tuesday, August 7, 2018

Abstract-Role of loss in all-dielectric metasurfaces



Andrew Cardin, Kebin Fan, Willie Padilla,

https://www.osapublishing.org/oe/abstract.cfm?uri=oe-26-13-17669&origin=search

Arrays of dielectric cylinders support two fundamental dipole active eigenmodes, which can be manipulated to elicit a variety of electromagnetic responses in all-dielectric metamaterials. Dissipation is a critical parameter in determining functionality; the present work varies material loss to explore the rich electromagnetic response of this class of metasurface. Four experimental cases are investigated which span electromagnetic response ranging from Huygens surfaces with transmissivity T = 94%, and phase ϕS21 = 235°, to metasurfaces which absorb 99.96% of incident energy. We find perfect absorption to be analogous to the driven damped harmonic oscillator, with critical damping occurring at resonance. With high phase contrast, transmission, and absorption all accessible from a single system, we present a uniquely diverse all-dielectric system.
© 2018 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

Thursday, May 3, 2018

Abstract-Flexible and tunable terahertz all-dielectric metasurface composed of ceramic spheres embedded in ferroelectric/ elastomer composite




Aleksandr Ushakov, Pavel Chizhov, Vladimir Bukin, Andrei Savel’ev, and Sergei Garnov

https://www.osapublishing.org/oe/abstract.cfm?uri=oe-26-9-11633


A pulsed broadband (from 0.1 to 1.5 THz), in-line, terahertz (THz) time domain electro-optical sampling is applied for the visualization of phase objects by using a large-aperture electro-optical crystal (ZnTe, ). The waveforms of the THz pulses are generated in a lithium niobate () crystal pumped by femtosecond pulses with a tilted amplitude front, and measured by a 2D THz imaging system. This system images the object under study in the THz range via a polytetrafluoroethylene (PTFE) lens in the  geometry onto a ZnTe crystal and then images the crystal surface on a CMOS camera using electro-optical sampling. Reconstruction of the image in such a scheme is implemented by processing the received 3D spatial-temporal distributions of the THz field in three different ways: (i) by detecting the displacement of the maximum peak position of the THz pulse due to a phase delay in the object under study; (ii) by using a cross-correlation function analysis; and (iii) by a Fourier transformation of a THz waveform and subsequent extraction of the phase difference at each THz frequency. Images of transparent PTFE objects were obtained. Main features of the resulting imaging system are discussed.

© 2018 Optical Society of America