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具有全光光束转向应用的时变梯度超表面。

Time-varying gradient metasurface with applications in all-optical beam steering.

作者信息

Karimi Mohammad, Alam M Zahirul, Upham Jeremy, Reshef Orad, Boyd Robert W

机构信息

School of Electrical Engineering and Computer Science, University of Ottawa, Ottawa, ON, K1N 6N5, Canada.

Department of Physics, University of Ottawa, Ottawa, ON, K1N 6N5, Canada.

出版信息

Nanophotonics. 2023 Mar 22;12(9):1733-1740. doi: 10.1515/nanoph-2022-0756. eCollection 2023 Apr.

DOI:10.1515/nanoph-2022-0756
PMID:39634111
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11501296/
Abstract

Integrating the large, subpicosecond nonlinear optical response of epsilon-near-zero (ENZ) materials with the broad design freedoms of plasmonic metasurfaces shows potential for creating rapidly modulated optical devices with possible applications in telecommunications, sensing, and reactive beam steering. In this work, we experimentally investigate a metasurface consisting of a plasmonic gradient array on a thin layer of indium tin oxide (ITO), characterize how incident probe pulses diffract from a system as it is being dynamically modulated by a pump pulse at wavelengths near the ENZ region. Angular shifts in the diffraction orders are observed and can be principally attributed to the adiabatic wavelength conversion of the probe as it witnesses the temporal change of index induced by the pump. Of note, the asymmetric gradient metasurface, considered to be a blazed diffraction grating, shows significantly different dynamic responses for different diffraction orders. The free-space wavelength shift to +1 and -1 diffraction orders is 6 and 12 nm, resulting in steering angle changes of 0.65 and 1.5°, respectively.

摘要

将ε近零(ENZ)材料的大的亚皮秒非线性光学响应与等离子体超表面广泛的设计自由度相结合,显示出制造快速调制光学器件的潜力,这些器件可能应用于电信、传感和反应光束控制。在这项工作中,我们通过实验研究了一种由氧化铟锡(ITO)薄层上的等离子体梯度阵列组成的超表面,表征了在接近ENZ区域的波长下,当入射探测脉冲被泵浦脉冲动态调制时,探测脉冲如何从该系统衍射。观察到衍射级次的角位移,这主要可归因于探测脉冲在见证泵浦引起的折射率随时间变化时的绝热波长转换。值得注意的是,被认为是闪耀衍射光栅的非对称梯度超表面,对于不同的衍射级次显示出显著不同的动态响应。自由空间波长向+1和-1衍射级次的偏移分别为6和12纳米,导致转向角变化分别为0.65和1.5°。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/bbc2949f6a44/j_nanoph-2022-0756_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/968f6454d8ce/j_nanoph-2022-0756_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/7e19caf54041/j_nanoph-2022-0756_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/2907a013c856/j_nanoph-2022-0756_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/bbc2949f6a44/j_nanoph-2022-0756_fig_004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/968f6454d8ce/j_nanoph-2022-0756_fig_001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/7e19caf54041/j_nanoph-2022-0756_fig_002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/2907a013c856/j_nanoph-2022-0756_fig_003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8c51/11501296/bbc2949f6a44/j_nanoph-2022-0756_fig_004.jpg

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Broadband frequency translation through time refraction in an epsilon-near-zero material.通过在近零介电常数材料中的时间折射实现宽带频率转换。
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