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Characteristics of Metal Enhanced Evanescent-Wave Microcavities

This article presents the concept of storing optical energy using a metallic air gap microcavity. Evanescent waves are stored in the air gap of a dielectric/metal/air gap/metal planar microcavity. For an air gap with a micron scale distance between the two metals, incident light excites the optical...

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Detalles Bibliográficos
Autor principal: Wakamatsu, Takashi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Molecular Diversity Preservation International (MDPI) 2010
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3231203/
https://www.ncbi.nlm.nih.gov/pubmed/22163684
http://dx.doi.org/10.3390/s100908751
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author Wakamatsu, Takashi
author_facet Wakamatsu, Takashi
author_sort Wakamatsu, Takashi
collection PubMed
description This article presents the concept of storing optical energy using a metallic air gap microcavity. Evanescent waves are stored in the air gap of a dielectric/metal/air gap/metal planar microcavity. For an air gap with a micron scale distance between the two metals, incident light excites the optical interface modes on the two metal-air interfaces simultaneously, being accompanied by enhanced evanescent fields. Numerical simulations show that the reflected light depends remarkably upon distributions of the enhanced electric fields in the air-gap at the optical mode excitations. The metallic microcavities have a Q value on the order of 10(2), as determined from calculations. Experimentally, a small mechanical variation of the air-gap distance exhibited a change of reflectivity.
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spelling pubmed-32312032011-12-07 Characteristics of Metal Enhanced Evanescent-Wave Microcavities Wakamatsu, Takashi Sensors (Basel) Article This article presents the concept of storing optical energy using a metallic air gap microcavity. Evanescent waves are stored in the air gap of a dielectric/metal/air gap/metal planar microcavity. For an air gap with a micron scale distance between the two metals, incident light excites the optical interface modes on the two metal-air interfaces simultaneously, being accompanied by enhanced evanescent fields. Numerical simulations show that the reflected light depends remarkably upon distributions of the enhanced electric fields in the air-gap at the optical mode excitations. The metallic microcavities have a Q value on the order of 10(2), as determined from calculations. Experimentally, a small mechanical variation of the air-gap distance exhibited a change of reflectivity. Molecular Diversity Preservation International (MDPI) 2010-09-21 /pmc/articles/PMC3231203/ /pubmed/22163684 http://dx.doi.org/10.3390/s100908751 Text en © 2010 by the authors; licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution license (http://creativecommons.org/licenses/by/3.0/).
spellingShingle Article
Wakamatsu, Takashi
Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title_full Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title_fullStr Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title_full_unstemmed Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title_short Characteristics of Metal Enhanced Evanescent-Wave Microcavities
title_sort characteristics of metal enhanced evanescent-wave microcavities
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3231203/
https://www.ncbi.nlm.nih.gov/pubmed/22163684
http://dx.doi.org/10.3390/s100908751
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