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Title: Antimatched Electromagnetic Metasurfaces for Broadband Arbitrary Phase Manipulation in Reflection

Abstract

Metasurfaces impart phase discontinuities on impinging electromagnetic waves that are typically limited to 0–2π. Here, we demonstrate that multiresonant metasurfaces can break free from this limitation and supply arbitrarily large, tunable time delays over ultrawide bandwidths. As such, ultrathin metasurfaces can act as the equivalent of thick bulk structures by emulating the multiple geometric resonances of three-dimensional systems that originate from phase accumulation with effective material resonances implemented on the surface itself via suitable subwavelength meta-atoms. We describe a constructive procedure for defining the required sheet admittivities of such metasurfaces. Importantly, the proposed approach provides an exactly linear phase response so that broadband pulses can experience the desired group delay without any distortion of the pulse shape. We focus on operation in reflection by exploiting an antimatching condition, satisfied by interleaved electric and magnetic Lorentzian resonances in the surface admittivities, which completely zeroes out transmission through the metasurface. As a result, the proposed metasurfaces can perfectly reflect a broadband pulse imparting a prescribed group delay. The group delay can be tuned by modifying the implemented resonances, thus opening up diverse possibilities in the temporal applications of metasurfaces.

Authors:
ORCiD logo [1];  [2];  [3]
  1. Institute of Electronic Structure and Laser, FORTH, GR-71110 Heraklion, Crete, Greece
  2. Ames Laboratory—U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, United States
  3. Institute of Electronic Structure and Laser, FORTH, GR-71110 Heraklion, Crete, Greece, Ames Laboratory—U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, United States
Publication Date:
Research Org.:
Ames Laboratory (AMES), Ames, IA (United States); Idryma Technologias kai Ereunas, Athens (Greece)
Sponsoring Org.:
USDOE; USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22). Materials Sciences & Engineering Division; European Union (EU)
OSTI Identifier:
1423697
Alternate Identifier(s):
OSTI ID: 1433662; OSTI ID: 1508574
Report Number(s):
IS-J-9616
Journal ID: ISSN 2330-4022
Grant/Contract Number:  
AC02-07CH11358; 736876; 320081
Resource Type:
Published Article
Journal Name:
ACS Photonics
Additional Journal Information:
Journal Name: ACS Photonics Journal Volume: 5 Journal Issue: 3; Journal ID: ISSN 2330-4022
Publisher:
American Chemical Society
Country of Publication:
United States
Language:
English
Subject:
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; 36 MATERIALS SCIENCE; metasurfaces; metamaterials; multiple resonances; tunable; broadband; reflection; phase delay; group delay

Citation Formats

Tsilipakos, Odysseas, Koschny, Thomas, and Soukoulis, Costas M. Antimatched Electromagnetic Metasurfaces for Broadband Arbitrary Phase Manipulation in Reflection. United States: N. p., 2018. Web. doi:10.1021/acsphotonics.7b01415.
Tsilipakos, Odysseas, Koschny, Thomas, & Soukoulis, Costas M. Antimatched Electromagnetic Metasurfaces for Broadband Arbitrary Phase Manipulation in Reflection. United States. https://doi.org/10.1021/acsphotonics.7b01415
Tsilipakos, Odysseas, Koschny, Thomas, and Soukoulis, Costas M. Wed . "Antimatched Electromagnetic Metasurfaces for Broadband Arbitrary Phase Manipulation in Reflection". United States. https://doi.org/10.1021/acsphotonics.7b01415.
@article{osti_1423697,
title = {Antimatched Electromagnetic Metasurfaces for Broadband Arbitrary Phase Manipulation in Reflection},
author = {Tsilipakos, Odysseas and Koschny, Thomas and Soukoulis, Costas M.},
abstractNote = {Metasurfaces impart phase discontinuities on impinging electromagnetic waves that are typically limited to 0–2π. Here, we demonstrate that multiresonant metasurfaces can break free from this limitation and supply arbitrarily large, tunable time delays over ultrawide bandwidths. As such, ultrathin metasurfaces can act as the equivalent of thick bulk structures by emulating the multiple geometric resonances of three-dimensional systems that originate from phase accumulation with effective material resonances implemented on the surface itself via suitable subwavelength meta-atoms. We describe a constructive procedure for defining the required sheet admittivities of such metasurfaces. Importantly, the proposed approach provides an exactly linear phase response so that broadband pulses can experience the desired group delay without any distortion of the pulse shape. We focus on operation in reflection by exploiting an antimatching condition, satisfied by interleaved electric and magnetic Lorentzian resonances in the surface admittivities, which completely zeroes out transmission through the metasurface. As a result, the proposed metasurfaces can perfectly reflect a broadband pulse imparting a prescribed group delay. The group delay can be tuned by modifying the implemented resonances, thus opening up diverse possibilities in the temporal applications of metasurfaces.},
doi = {10.1021/acsphotonics.7b01415},
journal = {ACS Photonics},
number = 3,
volume = 5,
place = {United States},
year = {Wed Jan 03 00:00:00 EST 2018},
month = {Wed Jan 03 00:00:00 EST 2018}
}

Journal Article:
Free Publicly Available Full Text
Publisher's Version of Record
https://doi.org/10.1021/acsphotonics.7b01415

Citation Metrics:
Cited by: 28 works
Citation information provided by
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Figures / Tables:

Figure 1. Figure 1.: Metasurface with resonant surface admittivities. (a) Adjacent resonances of the same kind (electric). The susceptivity zero crossing leads to a reflection minimum. The reflection phase is not monotonic. (b) Adjacent electric and magnetic resonances. Electric and magnetic susceptivities cannot compensate each other, and the reflection phase is monotonic.more » (c) Alternating electric and magnetic resonances. The magnetic resonance masks the electric susceptivity zero crossing. The reflection zero is avoided, and the reflection phase is monotonic. For the parameters of the Lorentzian resonances see the Supporting Information.« less

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Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.