The 2026 roadmap on wireless and microwave metasurfaces

Abstract Commonly, the electromagnetic properties of a microwave metamaterial are defined by its structure rather than by its chemical composition. Due to the nature of microwaves – electromagnetic radiation at frequencies between 300 MHz and 300 GHz – metamaterials are usually composed of a combination of conductive and dielectric materials, with subwavelength patterns defining how a wave interacts with it. A metamaterial which is very thin with respect to the operating wavelength is usually referred to as a metasurface. While the term “metamaterial” was first coined around the turn of the last millennium [1], antennas engineers have been designing engineered structures which would now be called metamaterials since at least the work of Ben Munk in the 1970s [2], and with the broadest definitions since artificial dielectric lenses were developed by Winston E. Kock at Bell Telephone Laboratories in the 1940s [3]. This historic link to telecommunications means similar techniques are used at lower frequencies, so this roadmap also includes metamaterials for other wireless applications.

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Publication Details

Journal
Journal of Physics D Applied Physics
Published
2025-12-11
DOI
https://doi.org/10.1088/1361-6463/ae2b7c
Primary Topic
Metamaterials and Metasurfaces Applications
Type
article
Field-Weighted Citation Impact
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article

The 2026 roadmap on wireless and microwave metasurfaces

Mustafa K. Taher Al‐Nuaimi, Fraser Burton, Farooq A. Tahir, Yangyishi Zhang et al.
Journal of Physics D Applied Physics
Metamaterials and Metasurfaces Applications
article

The 2026 roadmap on wireless and microwave metasurfaces

Mustafa K. Taher Al‐Nuaimi, Fraser Burton, Farooq A. Tahir, Yangyishi Zhang, Akram Alomainy, Milo Baraclough, Euan Humphreys, Miguel Navarro‐Cía, Stephen Henthorn, Qammer H. Abbasi, Alexander W. Powell, Imran Muhammad, Rupam Das, Syeda Fizzah Jilani, Jalil ur Rehman Kazim, William G. Whittow, Muhammad Aslam, Anikó Német, Aaron Walker
article en

Abstract

Abstract Commonly, the electromagnetic properties of a microwave metamaterial are defined by its structure rather than by its chemical composition. Due to the nature of microwaves – electromagnetic radiation at frequencies between 300 MHz and 300 GHz – metamaterials are usually composed of a combination of conductive and dielectric materials, with subwavelength patterns defining how a wave interacts with it. A metamaterial which is very thin with respect to the operating wavelength is usually referred to as a metasurface. While the term “metamaterial” was first coined around the turn of the last millennium [1], antennas engineers have been designing engineered structures which would now be called metamaterials since at least the work of Ben Munk in the 1970s [2], and with the broadest definitions since artificial dielectric lenses were developed by Winston E. Kock at Bell Telephone Laboratories in the 1940s [3]. This historic link to telecommunications means similar techniques are used at lower frequencies, so this roadmap also includes metamaterials for other wireless applications.

Journal of Physics D Applied Physics
BT Group (United Kingdom) (GB), Defence Science and Technology Laboratory (GB), Loughborough University (GB), Aberystwyth University (GB), Queen Mary University of London (GB), University of Exeter (GB), University of Glasgow (GB), University of Birmingham (GB), University of Sheffield (GB)
Openalex Percentile: Top 71%
Metamaterials and Metasurfaces Applications
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