Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna
Abstract We propose an axisymmetric silicon nanoresonator with designed tapered angle well for the extraordinary enhancement of the decay rate of magnetic dipole (MD) emitters. Due to the resonant coupling of a MD emitter and the MD mode of the subwavelength resonator, the Purcell factor (PF) can ea...
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2021-06-01
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Online Access: | https://doi.org/10.1038/s41598-021-92322-9 |
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doaj-9485e29e26a4442da58c55609a82049a2021-06-20T11:35:04ZengNature Publishing GroupScientific Reports2045-23222021-06-0111111110.1038/s41598-021-92322-9Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antennaMojtaba Karimi Habil0Carlos J. Zapata–Rodríguez1Mauro Cuevas2Samad Roshan Entezar3Faculty of Physics, University of TabrizDepartment of Optics and Optometry and Vision Sciences, University of ValenciaConsejo Nacional de Investigaciones Científicas y Técnicas (CONICET)Faculty of Physics, University of TabrizAbstract We propose an axisymmetric silicon nanoresonator with designed tapered angle well for the extraordinary enhancement of the decay rate of magnetic dipole (MD) emitters. Due to the resonant coupling of a MD emitter and the MD mode of the subwavelength resonator, the Purcell factor (PF) can easily reach 500, which is significantly higher than the PF when using a silicon nanosphere of the same size. The PF and the resonance frequency are conveniently tuned through the resonator diameter and the taper angle of the blind hole. When supported by a metallic substrate, further enhancement ( $$>10^3$$ > 10 3 ) of the MD spontaneous emission is triggered by an image-induced quadrupolar high-Q mode of the nanoantenna. For the sake of comparison we include a critical analysis of the canonical problem that considers a Si spherical shell. Our results might facilitate a novel strategy for promising realizations of chip-scale nanophotonic applications.https://doi.org/10.1038/s41598-021-92322-9 |
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DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Mojtaba Karimi Habil Carlos J. Zapata–Rodríguez Mauro Cuevas Samad Roshan Entezar |
spellingShingle |
Mojtaba Karimi Habil Carlos J. Zapata–Rodríguez Mauro Cuevas Samad Roshan Entezar Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna Scientific Reports |
author_facet |
Mojtaba Karimi Habil Carlos J. Zapata–Rodríguez Mauro Cuevas Samad Roshan Entezar |
author_sort |
Mojtaba Karimi Habil |
title |
Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
title_short |
Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
title_full |
Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
title_fullStr |
Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
title_full_unstemmed |
Multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
title_sort |
multipolar-sensitive engineering of magnetic dipole spontaneous emission with a dielectric nanoresonator antenna |
publisher |
Nature Publishing Group |
series |
Scientific Reports |
issn |
2045-2322 |
publishDate |
2021-06-01 |
description |
Abstract We propose an axisymmetric silicon nanoresonator with designed tapered angle well for the extraordinary enhancement of the decay rate of magnetic dipole (MD) emitters. Due to the resonant coupling of a MD emitter and the MD mode of the subwavelength resonator, the Purcell factor (PF) can easily reach 500, which is significantly higher than the PF when using a silicon nanosphere of the same size. The PF and the resonance frequency are conveniently tuned through the resonator diameter and the taper angle of the blind hole. When supported by a metallic substrate, further enhancement ( $$>10^3$$ > 10 3 ) of the MD spontaneous emission is triggered by an image-induced quadrupolar high-Q mode of the nanoantenna. For the sake of comparison we include a critical analysis of the canonical problem that considers a Si spherical shell. Our results might facilitate a novel strategy for promising realizations of chip-scale nanophotonic applications. |
url |
https://doi.org/10.1038/s41598-021-92322-9 |
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