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      Mirror‐Coupled Plasmonic Bound States in the Continuum for Tunable Perfect Absorption

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          Abstract

          Tailoring critical light‐matter coupling is a fundamental challenge of nanophotonics, impacting fields from higher harmonic generation and energy conversion to surface‐enhanced spectroscopy. Plasmonic perfect absorbers (PAs), where resonant antennas couple to their mirror images in adjacent metal films, excel at obtaining different coupling regimes by tuning the antenna‐film gap size. However, practical PA applications require constant gap size, making it impossible to maintain critical coupling beyond singular wavelengths. Here, a new approach for plasmonic PAs is introduced by combining mirror‐coupled resonances with the unique loss engineering capabilities of plasmonic quasi‐bound states in the continuum. This novel combination allows to tailor the light–matter interaction within the under‐coupling, over‐coupling, and critical coupling regimes using flexible tuning knobs including asymmetry parameter, dielectric gap, and geometrical scaling factor. The study demonstrates a pixelated PA metasurface with optimal absorption over a broad range of mid‐infrared wavenumbers (950–2000 cm −1) using only a single gap size and applies it for multispectral surface‐enhanced molecular spectroscopy. Moreover, the asymmetry parameter enables convenient adjustment of the quality factor and resonance amplitude. This concept expands the capabilities and flexibility of traditional gap‐tuned PAs, opening new perspectives for miniaturized sensing platforms towards on‐chip and in situ detection.

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          Most cited references59

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          Perfect metamaterial absorber.

          We present the design for an absorbing metamaterial (MM) with near unity absorbance A(omega). Our structure consists of two MM resonators that couple separately to electric and magnetic fields so as to absorb all incident radiation within a single unit cell layer. We fabricate, characterize, and analyze a MM absorber with a slightly lower predicted A(omega) of 96%. Unlike conventional absorbers, our MM consists solely of metallic elements. The substrate can therefore be optimized for other parameters of interest. We experimentally demonstrate a peak A(omega) greater than 88% at 11.5 GHz.
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            Taming the blackbody with infrared metamaterials as selective thermal emitters.

            In this Letter we demonstrate, for the first time, selective thermal emitters based on metamaterial perfect absorbers. We experimentally realize a narrow band midinfrared (MIR) thermal emitter. Multiple metamaterial sublattices further permit construction of a dual-band MIR emitter. By performing both emissivity and absorptivity measurements, we find that emissivity and absorptivity agree very well as predicted by Kirchhoff's law of thermal radiation. Our results directly demonstrate the great flexibility of metamaterials for tailoring blackbody emission.
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              Asymmetric Metasurfaces with High- \(Q\) Resonances Governed by Bound States in the Continuum

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                Author and article information

                Contributors
                (View ORCID Profile)
                Journal
                Laser & Photonics Reviews
                Laser & Photonics Reviews
                Wiley
                1863-8880
                1863-8899
                November 2023
                August 27 2023
                November 2023
                : 17
                : 11
                Affiliations
                [1 ] Chair in Hybrid Nanosystems Nanoinstitute Munich Faculty of Physics Ludwig‐Maximilians‐Universität München 80539 München Germany
                [2 ] School of Physics and Astronomy Monash University Clayton Victoria 3800 Australia
                [3 ] The Blackett Laboratory Department of Physics Imperial College London London SW7 2AZ UK
                Article
                10.1002/lpor.202300294
                d9e9d18c-231c-4cf7-b49b-ea4fb1b569b5
                © 2023

                http://creativecommons.org/licenses/by/4.0/

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