A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router
Abstract Geometric metasurfaces primarily follow the physical mechanism of Pancharatnam–Berry (PB) phases, empowering wavefront control of cross‐polarized reflective/transmissive light components. However, inherently accompanying the cross‐polarized components, the copolarized output components have...
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doaj-21a9d315a8b4420ebb1b44431ac222bc2020-11-25T03:42:33ZengWileyAdvanced Science2198-38442020-09-01718n/an/a10.1002/advs.202001437A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization RouterYueyi Yuan0Shang Sun1Yang Chen2Kuang Zhang3Xumin Ding4Badreddine Ratni5Qun Wu6Shah Nawaz Burokur7Cheng‐Wei Qiu8Department of Microwave Engineering Harbin Institute of Technology Harbin 150001 ChinaDepartment of Electrical and Computer Engineering National University of Singapore Singapore 117583 SingaporeDepartment of Electrical and Computer Engineering National University of Singapore Singapore 117583 SingaporeDepartment of Microwave Engineering Harbin Institute of Technology Harbin 150001 ChinaDepartment of Microwave Engineering Harbin Institute of Technology Harbin 150001 ChinaLEME, UPL Univ Paris Nanterre Ville‐d'Avray F92410 FranceDepartment of Microwave Engineering Harbin Institute of Technology Harbin 150001 ChinaLEME, UPL Univ Paris Nanterre Ville‐d'Avray F92410 FranceDepartment of Electrical and Computer Engineering National University of Singapore Singapore 117583 SingaporeAbstract Geometric metasurfaces primarily follow the physical mechanism of Pancharatnam–Berry (PB) phases, empowering wavefront control of cross‐polarized reflective/transmissive light components. However, inherently accompanying the cross‐polarized components, the copolarized output components have not been attempted in parallel in existing works. Here, a general method is proposed to construct phase‐modulated metasurfaces for implementing functionalities separately in co‐ and cross‐polarized output fields under circularly polarized (CP) incidence, which is impossible to achieve with solely a geometric phase. By introducing a propagation phase as an additional degree of freedom, the electromagnetic (EM) energy carried by co‐ and cross‐polarized transmitted fields can be fully phase‐modulated with independent wavefronts. Under one CP incidence, a metasurface for separate functionalities with controllable energy repartition is verified by simulations and proof‐of‐principle microwave experiments. A variety of applications can be readily expected in spin‐selective optics, spin‐Hall metasurfaces, and multitasked metasurfaces operating in both reflective and transmissive modes.https://doi.org/10.1002/advs.202001437circular polarizationenergy‐controlmetasurfacesphase modulationrouters |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yueyi Yuan Shang Sun Yang Chen Kuang Zhang Xumin Ding Badreddine Ratni Qun Wu Shah Nawaz Burokur Cheng‐Wei Qiu |
spellingShingle |
Yueyi Yuan Shang Sun Yang Chen Kuang Zhang Xumin Ding Badreddine Ratni Qun Wu Shah Nawaz Burokur Cheng‐Wei Qiu A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router Advanced Science circular polarization energy‐control metasurfaces phase modulation routers |
author_facet |
Yueyi Yuan Shang Sun Yang Chen Kuang Zhang Xumin Ding Badreddine Ratni Qun Wu Shah Nawaz Burokur Cheng‐Wei Qiu |
author_sort |
Yueyi Yuan |
title |
A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router |
title_short |
A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router |
title_full |
A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router |
title_fullStr |
A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router |
title_full_unstemmed |
A Fully Phase‐Modulated Metasurface as An Energy‐Controllable Circular Polarization Router |
title_sort |
fully phase‐modulated metasurface as an energy‐controllable circular polarization router |
publisher |
Wiley |
series |
Advanced Science |
issn |
2198-3844 |
publishDate |
2020-09-01 |
description |
Abstract Geometric metasurfaces primarily follow the physical mechanism of Pancharatnam–Berry (PB) phases, empowering wavefront control of cross‐polarized reflective/transmissive light components. However, inherently accompanying the cross‐polarized components, the copolarized output components have not been attempted in parallel in existing works. Here, a general method is proposed to construct phase‐modulated metasurfaces for implementing functionalities separately in co‐ and cross‐polarized output fields under circularly polarized (CP) incidence, which is impossible to achieve with solely a geometric phase. By introducing a propagation phase as an additional degree of freedom, the electromagnetic (EM) energy carried by co‐ and cross‐polarized transmitted fields can be fully phase‐modulated with independent wavefronts. Under one CP incidence, a metasurface for separate functionalities with controllable energy repartition is verified by simulations and proof‐of‐principle microwave experiments. A variety of applications can be readily expected in spin‐selective optics, spin‐Hall metasurfaces, and multitasked metasurfaces operating in both reflective and transmissive modes. |
topic |
circular polarization energy‐control metasurfaces phase modulation routers |
url |
https://doi.org/10.1002/advs.202001437 |
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