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Ultrathin 3R-MoS$_2$ metasurfaces with atomically precise edges for efficient nonlinear nanophotonics

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arxiv 2410.20960 v1 pith:N5V2QCH3 submitted 2024-10-28 physics.optics cond-mat.mtrl-sci

classification physics.opticscond-mat.mtrl-sci
keywords metasurfacesedgesatomicallyetchingmaterialsnonlinearitiesopticalprecise
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abstract

Dielectric metasurfaces that combine high-index materials with optical nonlinearities are widely recognized for their potential in various quantum and classical nanophotonic applications. However, the fabrication of high-quality metasurfaces poses significant material-dependent challenges, as their designs are often susceptible to disorder, defects, and scattering losses, which are particularly prone to occur at the edges of nanostructured features. Additionally, the choice of the material platforms featuring second-order optical nonlinearities, $\chi^{(2)}$, is limited to broken-inversion symmetry crystals such as GaAs, GaP, LiNbO$_3$, and various bulk van der Waals materials, including GaSe and NbOCl$_2$. Here, we use a combination of top-down lithography and anisotropic wet etching of a specially stacked van der Waals crystal -- 3R-MoS$_2$, which exhibits both a high refractive index and exceptional $\chi^{(2)}$ nonlinearity, to produce metasurfaces consisting of perfect equilateral triangle nanoholes with atomically precise zigzag edges. Due to the geometry of the triangle, the etching process is accompanied by a transition from an in-plane $C_4$ symmetric structure to a broken-in-plane symmetry configuration, thereby allowing for the realization of the quasi-bound-state-in-the-continuum (q-BIC) concept. The resulting ultrathin metasurface ($\sim$ 20-25 nm) demonstrates a remarkable enhancement in second-harmonic generation (SHG) -- over three orders of magnitude at specific wavelengths and linear polarization directions compared to a host flake.

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  1. Dynamic Control of Nonlinear Emission by Exciton-Photon Coupling in WS2 Metasurfaces

    physics.optics 2025-06 conditional novelty 6.0 of 10

    A qBIC WS2 crescent metasurface with resonance at twice the exciton energy yields 98-fold stronger SHG than monolayer WS2, 4 orders of magnitude stronger than unpatterned film, tunable by temperature and polarization.

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