Incomplete phase metasurface for wavefront reconstruction

Metasurfaces consisting of subwavelength elements exhibit unparalleled flexibility in light manipulation in terms of phase, amplitude, and/or polarization at ultrathin dimensions. Typically, a continuous and complete phase distribution covering a full 2π range is required in metasurface design to pr...

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Main Authors: Liu, Qiyao, Liu, Zhengtong, Ma, Xuezhi, Deng, Jie, Zhang, Chen, Chen, Zhenmin, Nemati, Arash, Ng, Sui Kit, Gorelik, Sergey, Teo, Siew Lang, Ji, Rong, Zhao, Meng, Gonzaga, Leonard Verano, Liu, Hong, Yue, Fuyong, Yu, Shaohua, Luo, Yu, Wang,Qian
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2024
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Online Access:https://hdl.handle.net/10356/179134
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-1791342024-07-26T15:40:02Z Incomplete phase metasurface for wavefront reconstruction Liu, Qiyao Liu, Zhengtong Ma, Xuezhi Deng, Jie Zhang, Chen Chen, Zhenmin Nemati, Arash Ng, Sui Kit Gorelik, Sergey Teo, Siew Lang Ji, Rong Zhao, Meng Gonzaga, Leonard Verano Liu, Hong Yue, Fuyong Yu, Shaohua Luo, Yu Wang,Qian School of Electrical and Electronic Engineering Institute of Materials Research and Engineering, A*STAR Centre for OptoElectronics and Biophotonics Engineering Incomplete phase metasurface Metagrating Metalens Flatoptics Polarizationinsensitive Metasurfaces consisting of subwavelength elements exhibit unparalleled flexibility in light manipulation in terms of phase, amplitude, and/or polarization at ultrathin dimensions. Typically, a continuous and complete phase distribution covering a full 2π range is required in metasurface design to produce the performance of conventional optical components, such as gratings, lenses, and beam splitters. However, an incomplete phase, i.e., with phase change less or larger than 2π, can provide additional degrees of freedom for optical wavefront reconstruction. This article shows that designed metagratings, which unlocked the 2π phase constraint in supercell designs, achieved arbitrary control of the intensity ratio between any adjacent diffraction orders, while keeping the diffraction directions consistent with those of conventional gratings. Four metagratings, as representatives, with different phase ranges in the supercell, i.e., π, 2π, 3π, and 4π, have been designed and fabricated to demonstrate the diffraction intensity redistribution capability of metagratings. The 0th- and the 1st-order splitting ratios measured in experiments can reach 0.07 to 24.8, which is a hard task for traditional grating devices. Using a simple design methodology, incomplete phase metasurfaces hold great promise for developing various functional ultrathin nanophotonic devices, such as controllable beam splitters, spectrometers, and multifoci metalens. Agency for Science, Technology and Research (A*STAR) Submitted/Accepted version This research was supported by the Agency for Science, Technology and Research (A*STAR) under its AME IRG Fund (Grant No. A20E5c0095, M22K2c0080), Career Development Fund (Grant No. C210112044 and C210812027), Career Development Fund-Seed Projects (Grant No. 222D800038), and AME programmatic Fund (Grant No. A18A7b0058). This research was also supported by the Major Key Project of PCL, and the Talent Program of Guangdong Province (Grant No. 2021CX02X465). 2024-07-22T04:42:36Z 2024-07-22T04:42:36Z 2023 Journal Article Liu, Q., Liu, Z., Ma, X., Deng, J., Zhang, C., Chen, Z., Nemati, A., Ng, S. K., Gorelik, S., Teo, S. L., Ji, R., Zhao, M., Gonzaga, L. V., Liu, H., Yue, F., Yu, S., Luo, Y. & Wang, Q. (2023). Incomplete phase metasurface for wavefront reconstruction. ACS Photonics, 10(8), 2563-2569. https://dx.doi.org/10.1021/acsphotonics.3c00275 2330-4022 https://hdl.handle.net/10356/179134 10.1021/acsphotonics.3c00275 2-s2.0-85165924756 8 10 2563 2569 en A20E5c0095 M22K2c0080 C210112044 C210812027 222D800038 A18A7b0058 ACS Photonics © 2023 American Chemical Society. All rights reserved. This article may be downloaded for personal use only. Any other use requires prior permission of the copyright holder. The Version of Record is available online at http://doi.org/10.1021/acsphotonics.3c00275. application/pdf
institution Nanyang Technological University
building NTU Library
continent Asia
country Singapore
Singapore
content_provider NTU Library
collection DR-NTU
language English
topic Engineering
Incomplete phase metasurface
Metagrating
Metalens
Flatoptics
Polarizationinsensitive
spellingShingle Engineering
Incomplete phase metasurface
Metagrating
Metalens
Flatoptics
Polarizationinsensitive
Liu, Qiyao
Liu, Zhengtong
Ma, Xuezhi
Deng, Jie
Zhang, Chen
Chen, Zhenmin
Nemati, Arash
Ng, Sui Kit
Gorelik, Sergey
Teo, Siew Lang
Ji, Rong
Zhao, Meng
Gonzaga, Leonard Verano
Liu, Hong
Yue, Fuyong
Yu, Shaohua
Luo, Yu
Wang,Qian
Incomplete phase metasurface for wavefront reconstruction
description Metasurfaces consisting of subwavelength elements exhibit unparalleled flexibility in light manipulation in terms of phase, amplitude, and/or polarization at ultrathin dimensions. Typically, a continuous and complete phase distribution covering a full 2π range is required in metasurface design to produce the performance of conventional optical components, such as gratings, lenses, and beam splitters. However, an incomplete phase, i.e., with phase change less or larger than 2π, can provide additional degrees of freedom for optical wavefront reconstruction. This article shows that designed metagratings, which unlocked the 2π phase constraint in supercell designs, achieved arbitrary control of the intensity ratio between any adjacent diffraction orders, while keeping the diffraction directions consistent with those of conventional gratings. Four metagratings, as representatives, with different phase ranges in the supercell, i.e., π, 2π, 3π, and 4π, have been designed and fabricated to demonstrate the diffraction intensity redistribution capability of metagratings. The 0th- and the 1st-order splitting ratios measured in experiments can reach 0.07 to 24.8, which is a hard task for traditional grating devices. Using a simple design methodology, incomplete phase metasurfaces hold great promise for developing various functional ultrathin nanophotonic devices, such as controllable beam splitters, spectrometers, and multifoci metalens.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Liu, Qiyao
Liu, Zhengtong
Ma, Xuezhi
Deng, Jie
Zhang, Chen
Chen, Zhenmin
Nemati, Arash
Ng, Sui Kit
Gorelik, Sergey
Teo, Siew Lang
Ji, Rong
Zhao, Meng
Gonzaga, Leonard Verano
Liu, Hong
Yue, Fuyong
Yu, Shaohua
Luo, Yu
Wang,Qian
format Article
author Liu, Qiyao
Liu, Zhengtong
Ma, Xuezhi
Deng, Jie
Zhang, Chen
Chen, Zhenmin
Nemati, Arash
Ng, Sui Kit
Gorelik, Sergey
Teo, Siew Lang
Ji, Rong
Zhao, Meng
Gonzaga, Leonard Verano
Liu, Hong
Yue, Fuyong
Yu, Shaohua
Luo, Yu
Wang,Qian
author_sort Liu, Qiyao
title Incomplete phase metasurface for wavefront reconstruction
title_short Incomplete phase metasurface for wavefront reconstruction
title_full Incomplete phase metasurface for wavefront reconstruction
title_fullStr Incomplete phase metasurface for wavefront reconstruction
title_full_unstemmed Incomplete phase metasurface for wavefront reconstruction
title_sort incomplete phase metasurface for wavefront reconstruction
publishDate 2024
url https://hdl.handle.net/10356/179134
_version_ 1814047201911898112