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Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)

This article reports the finding of the plasmonic induced polarization rotation and propagation rotation when the plane EM wave radiates the adjacent active coated nano particle and large dielectric sphere at resonant frequency. The results investigate that the incident electromagnetic planewave exc...

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Autores principales: Hayat, Qaisar, Geng, Junping, Liang, Xianling, Jin, Ronghong, Hayat, Khizar, He, Chong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7028718/
https://www.ncbi.nlm.nih.gov/pubmed/32071332
http://dx.doi.org/10.1038/s41598-020-59621-z
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author Hayat, Qaisar
Geng, Junping
Liang, Xianling
Jin, Ronghong
Hayat, Khizar
He, Chong
author_facet Hayat, Qaisar
Geng, Junping
Liang, Xianling
Jin, Ronghong
Hayat, Khizar
He, Chong
author_sort Hayat, Qaisar
collection PubMed
description This article reports the finding of the plasmonic induced polarization rotation and propagation rotation when the plane EM wave radiates the adjacent active coated nano particle and large dielectric sphere at resonant frequency. The results investigate that the incident electromagnetic planewave excites the TM(21) mode in the large size dielectric sphere at first, which affects the TM(11) mode field from the coated nano particle. Consequently, when the combined active coated nano particle and large dielectric sphere are in resonant, the main E–field polarization direction becomes parallel to the propagation direction of the original planewave and main beam of the pattern becomes omnidirectional i.e. both rotates by 90°. Furthermore, the polarization and propagation rotation angle varies with different size of the dielectric sphere. Likewise, the structure of dielectric sphere clamped by two active nanoparticles is also showing plasmonic induced polarization and propagation rotation along with TM(11) mode from each coated nano particle (CNP) having 180° phase difference. In addition to this, the induced polarization rotation was also verified by the Electric Hertzian Dipole (EHD). The integration of this simpler geometry with other optical devices has possible applications in polarization manipulation, nano-sensors and detectors on nanoscale.
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spelling pubmed-70287182020-02-26 Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR) Hayat, Qaisar Geng, Junping Liang, Xianling Jin, Ronghong Hayat, Khizar He, Chong Sci Rep Article This article reports the finding of the plasmonic induced polarization rotation and propagation rotation when the plane EM wave radiates the adjacent active coated nano particle and large dielectric sphere at resonant frequency. The results investigate that the incident electromagnetic planewave excites the TM(21) mode in the large size dielectric sphere at first, which affects the TM(11) mode field from the coated nano particle. Consequently, when the combined active coated nano particle and large dielectric sphere are in resonant, the main E–field polarization direction becomes parallel to the propagation direction of the original planewave and main beam of the pattern becomes omnidirectional i.e. both rotates by 90°. Furthermore, the polarization and propagation rotation angle varies with different size of the dielectric sphere. Likewise, the structure of dielectric sphere clamped by two active nanoparticles is also showing plasmonic induced polarization and propagation rotation along with TM(11) mode from each coated nano particle (CNP) having 180° phase difference. In addition to this, the induced polarization rotation was also verified by the Electric Hertzian Dipole (EHD). The integration of this simpler geometry with other optical devices has possible applications in polarization manipulation, nano-sensors and detectors on nanoscale. Nature Publishing Group UK 2020-02-18 /pmc/articles/PMC7028718/ /pubmed/32071332 http://dx.doi.org/10.1038/s41598-020-59621-z Text en © The Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Hayat, Qaisar
Geng, Junping
Liang, Xianling
Jin, Ronghong
Hayat, Khizar
He, Chong
Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title_full Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title_fullStr Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title_full_unstemmed Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title_short Subwavelength plasmonic nanoantenna as a Plasmonic Induced Polarization Rotator (PI-PR)
title_sort subwavelength plasmonic nanoantenna as a plasmonic induced polarization rotator (pi-pr)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7028718/
https://www.ncbi.nlm.nih.gov/pubmed/32071332
http://dx.doi.org/10.1038/s41598-020-59621-z
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