Abstract

AbstractPlasmonic metasurfaces, which can be considered as the two-dimensional analog of metal-based metamaterials, have attracted progressively increasing attention in recent years because of the ease of fabrication and unprecedented control over the reflected or transmitted light while featuring relatively low losses even at optical wavelengths. Among all the different design approaches, gap-surface plasmon metasurfaces – a specific branch of plasmonic metasurfaces – which consist of a subwavelength thin dielectric spacer sandwiched between an optically thick metal film and arrays of metal subwavelength elements arranged in a strictly or quasi-periodic fashion, have gained awareness from researchers working at practically any frequency regime as its realization only requires a single lithographic step, yet with the possibility to fully control the amplitude, phase, and polarization of the reflected light. In this paper, we review the fundamentals, recent developments, and opportunities of gap-surface plasmon metasurfaces. Starting with introducing the concept of gap-surface plasmon metasurfaces, we present three typical gap-surface plasmon resonators, introduce generalized Snell’s law, and explain the concept of Pancharatnam-Berry phase. We then overview the main applications of gap-surface plasmon metasurfaces, including beam-steerers, flat lenses, holograms, absorbers, color printing, polarization control, surface wave couplers, and dynamically reconfigurable metasurfaces. The review is ended with a short summary and outlook on possible future developments.

Highlights

  • The capability of manipulating light at will is tantalizingly attractive, promising numerous applications

  • Gap-surface plasmon metasurfaces (GSPMs) – a specific branch of plasmonic metasurfaces – which consist of a subwavelength thin dielectric spacer sandwiched between an optically thick metal film and arrays of metal subwavelength elements arranged in a strictly or quasi-periodic fashion, have gained awareness from researchers working at practically any frequency regime as its realization only requires a single lithographic step, yet with the possibility to fully control the amplitude, phase, and polarization of the reflected light

  • In addition to manipulating the propagating waves (PWs) in free space, another exciting feature of gap-surface plasmon metasurfaces (GSPMs) is the capability of efficiently launching surface waves (SWs), such as SPPs and spoof SPPs in low-frequency range, in which arbitrary in-plane wave vector can be designed to match with the wave vector of SWs, distinct from the prism or grating couplers based on resonant coupling between PW and SW [155]

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Summary

Introduction

The capability of manipulating light at will is tantalizingly attractive, promising numerous applications. Conventional methods to mold the flow of light are typically relying on gradually accumulated amplitude, phase, and polarization changes during light propagation [1], with the resulting devices featuring certain curved surfaces and complex shapes. These bulky configurations do not comply with current trends aiming at very dense integration and miniaturization in photonics/plasmonics. Gap-surface plasmon metasurfaces (GSPMs) – a specific branch of plasmonic metasurfaces – which consist of a subwavelength thin dielectric spacer sandwiched between an optically thick metal film and arrays of metal subwavelength elements arranged in a strictly or quasi-periodic fashion, have gained awareness from researchers working at practically any frequency regime as its realization only requires a single lithographic step, yet with the possibility to fully control the amplitude, phase, and polarization of the reflected light.

GSP resonator
Generalized Snell’s law
PB phase
Applications of GSPMs
Beam steering
Planar metalens
GSPM-based hologram
Broadband absorbers
High-resolution color printing
Polarimeter control
Polarimeter detection
S urface wave couplers
D ynamically reconfigurable GSPMs
Other applications
Findings
Conclusions and outlook
Full Text
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