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A broadband achromatic metalens array for integral imaging in the visible

机译:用于可见光中整体成像的宽带消色差金属元阵列

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摘要

Integral imaging is a promising three-dimensional (3D) imaging technique that captures and reconstructs light field information.Microlens arrays are usually used for the reconstruction process to display 3D scenes to the viewer.However,the inherent chromatic aberration of the microlens array reduces the viewing quality,and thus,broadband achromatic imaging remains a challenge for integral imaging.Here,we realize a silicon nitride metalens array in the visible region that can be used to reconstruct 3D optical scenes in the achromatic integral imaging for white light.The metalens array contains 60 × 60 polarization-insensitive metalenses with nearly diffraction-limited focusing.The nanoposts in each high-efficiency (measured as 47% on average) metalens are delicately designed with zero effective material dispersion and an effective achromatic refractive index distribution from 430 to 780 nm.In addition,such an achromatic metalens array is composed of only a single silicon nitride layer with an ultrathin thickness of 400 nm,making the array suitable for on-chip hybrid-CMOS integration and the parallel manipulation of optoelectronic information.We expect these findings to provide possibilities for full-color and aberration-free integral imaging,and we envision that the proposed approach may be potentially applicable in the fields of high-power microlithography,high-precision wavefront sensors,virtual/augmented reality and 3D imaging.
机译:整体成像是一种有前途的三维(3D)成像技术,可以捕获和重建光场信息。微透镜阵列通常用于重建过程中向观看者显示3D场景,但是微透镜阵列的固有色差会降低观看质量,因此,宽带消色差成像仍然是积分成像的挑战。在这里,我们实现了在可见光区域的氮化硅金属阵列,可用于在白光消色差积分成像中重建3D光学场景。包含60×60个对偏振不敏感的金属感镜,具有接近衍射极限的聚焦。每个高效(平均测得47%)金属素中的纳米柱均经过精心设计,有效材料分散为零,有效消色差折射率分布在430至780之间此外,这种消色差金属阵列仅由单个氮化硅层w 400 nm的超薄厚度,使得该阵列适用于片上混合CMOS集成和光电信息的并行处理。我们希望这些发现将为全色和无像差的集成成像提供可能性,并且我们认为所提出的方法可能潜在地适用于大功率微光刻,高精度波前传感器,虚拟/增强现实和3D成像领域。

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  • 来源
    《光:科学与应用(英文版)》 |2019年第4期|600-609|共10页
  • 作者单位

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    School of Physics, Sun Yat-sen University, Guangzhou 510275, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    School of Physics, Sun Yat-sen University, Guangzhou 510275, China;

    School of Instrumentation and Optoelectronic Engineering, Beihang University, Beijing 100191, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    School of Physics, Sun Yat-sen University, Guangzhou 510275, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    School of Instrumentation and Optoelectronic Engineering, Beihang University, Beijing 100191, China;

    School of Instrumentation and Optoelectronic Engineering, Beihang University, Beijing 100191, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-sen University, Guangzhou 510275, China;

    School of Physics, Sun Yat-sen University, Guangzhou 510275, China;

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  • 入库时间 2024-01-27 00:23:53
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