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      Helical Structure Endows Liquid Crystal Planar Optics with a Customizable Working Band

      1 , 1 , 2 , 1
      Advanced Quantum Technologies
      Wiley

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          Abstract

          Wavefront control lies in the heart of optics. Multi‐degree orthogonal manipulation of light, especially the on‐demand tailoring of the working band and spatial phase front, is expected to fully exhibit the superiority of photons as information carriers. Here, the recent progress on the customizable working band of liquid crystal planar optics enabled by helical structures is reviewed. Broadband transmissive devices with mirror‐symmetric helical structures, broadband reflective Bragg‐Berry phase elements based on cholesteric liquid crystals, transflective phase modulations of a piecewise twisted structure, and external field shifted bands of planar optics are summarized. In addition to the customization of the geometric phase and working band, manipulation of other optical parameters is discussed. The tremendous self‐assemblies and diverse external field responsiveness make liquid crystals a perfect platform for full‐dimensional manipulation of light.

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          Most cited references92

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          Light propagation with phase discontinuities: generalized laws of reflection and refraction.

          Conventional optical components rely on gradual phase shifts accumulated during light propagation to shape light beams. New degrees of freedom are attained by introducing abrupt phase changes over the scale of the wavelength. A two-dimensional array of optical resonators with spatially varying phase response and subwavelength separation can imprint such phase discontinuities on propagating light as it traverses the interface between two media. Anomalous reflection and refraction phenomena are observed in this regime in optically thin arrays of metallic antennas on silicon with a linear phase variation along the interface, which are in excellent agreement with generalized laws derived from Fermat's principle. Phase discontinuities provide great flexibility in the design of light beams, as illustrated by the generation of optical vortices through use of planar designer metallic interfaces.
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            Flat optics with designer metasurfaces.

            Conventional optical components such as lenses, waveplates and holograms rely on light propagation over distances much larger than the wavelength to shape wavefronts. In this way substantial changes of the amplitude, phase or polarization of light waves are gradually accumulated along the optical path. This Review focuses on recent developments on flat, ultrathin optical components dubbed 'metasurfaces' that produce abrupt changes over the scale of the free-space wavelength in the phase, amplitude and/or polarization of a light beam. Metasurfaces are generally created by assembling arrays of miniature, anisotropic light scatterers (that is, resonators such as optical antennas). The spacing between antennas and their dimensions are much smaller than the wavelength. As a result the metasurfaces, on account of Huygens principle, are able to mould optical wavefronts into arbitrary shapes with subwavelength resolution by introducing spatial variations in the optical response of the light scatterers. Such gradient metasurfaces go beyond the well-established technology of frequency selective surfaces made of periodic structures and are extending to new spectral regions the functionalities of conventional microwave and millimetre-wave transmit-arrays and reflect-arrays. Metasurfaces can also be created by using ultrathin films of materials with large optical losses. By using the controllable abrupt phase shifts associated with reflection or transmission of light waves at the interface between lossy materials, such metasurfaces operate like optically thin cavities that strongly modify the light spectrum. Technology opportunities in various spectral regions and their potential advantages in replacing existing optical components are discussed.
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              Metasurface holograms reaching 80% efficiency.

              Surfaces covered by ultrathin plasmonic structures--so-called metasurfaces--have recently been shown to be capable of completely controlling the phase of light, representing a new paradigm for the design of innovative optical elements such as ultrathin flat lenses, directional couplers for surface plasmon polaritons and wave plate vortex beam generation. Among the various types of metasurfaces, geometric metasurfaces, which consist of an array of plasmonic nanorods with spatially varying orientations, have shown superior phase control due to the geometric nature of their phase profile. Metasurfaces have recently been used to make computer-generated holograms, but the hologram efficiency remained too low at visible wavelengths for practical purposes. Here, we report the design and realization of a geometric metasurface hologram reaching diffraction efficiencies of 80% at 825 nm and a broad bandwidth between 630 nm and 1,050 nm. The 16-level-phase computer-generated hologram demonstrated here combines the advantages of a geometric metasurface for the superior control of the phase profile and of reflectarrays for achieving high polarization conversion efficiency. Specifically, the design of the hologram integrates a ground metal plane with a geometric metasurface that enhances the conversion efficiency between the two circular polarization states, leading to high diffraction efficiency without complicating the fabrication process. Because of these advantages, our strategy could be viable for various practical holographic applications.
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                Author and article information

                Contributors
                Journal
                Advanced Quantum Technologies
                Adv Quantum Tech
                Wiley
                2511-9044
                2511-9044
                February 2023
                January 11 2023
                February 2023
                : 6
                : 2
                Affiliations
                [1 ]College of Engineering and Applied Sciences Nanjing University Nanjing 210023 China
                [2 ]Department of Chemistry Tsinghua University Beijing 100084 China
                Article
                10.1002/qute.202200153
                8466178d-f3f9-4e14-9b7a-90f1aabcec5b
                © 2023

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