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Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor

Dielectric grating-based sensors are usually based on the guided mode resonance (GMR) obtained using a thin planar waveguide layer (PWL) adjacent to a thin subwavelength grating layer. In this work, we present a detailed investigation of thick subwavelength dielectric grating structures that exhibit...

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Detalles Bibliográficos
Autores principales: Isaacs, Sivan, Hajoj, Ansar, Abutoama, Mohammad, Kozlovsky, Alexander, Golan, Erez, Abdulhalim, Ibrahim
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6651248/
https://www.ncbi.nlm.nih.gov/pubmed/31288404
http://dx.doi.org/10.3390/s19133003
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author Isaacs, Sivan
Hajoj, Ansar
Abutoama, Mohammad
Kozlovsky, Alexander
Golan, Erez
Abdulhalim, Ibrahim
author_facet Isaacs, Sivan
Hajoj, Ansar
Abutoama, Mohammad
Kozlovsky, Alexander
Golan, Erez
Abdulhalim, Ibrahim
author_sort Isaacs, Sivan
collection PubMed
description Dielectric grating-based sensors are usually based on the guided mode resonance (GMR) obtained using a thin planar waveguide layer (PWL) adjacent to a thin subwavelength grating layer. In this work, we present a detailed investigation of thick subwavelength dielectric grating structures that exhibit reflection resonances above a certain thickness without the need for the waveguide layer, showing great potential for applications in biosensing and tunable filtering. Analytic and numerical results are thoroughly discussed, as well as an experimental demonstration of the structure as a chemical sensor in the SWIR (short wave infrared) spectral range (1200–1800 nm). In comparison to the GMR structure with PWL, the thick grating structure has several unique properties: (i) It gives higher sensitivity when the spaces are filled, with the analyte peaking at certain space values due to an increase in the interaction volume between the analyte and the evanescent optical field between the grating lines; (ii) the TM (transverse magnetic) resonance, in certain cases, provides a better figure of merit; (iii) the sensitivity increases as the grating height increases; (iv) the prediction of the resonance locations based on the effective medium approximation does not give satisfactory results when the grating height is larger than a certain value, and the invalidity becomes more severe as the period increases; (v) a sudden increase in the Q-factor of the resonance occurs at a specific height value accompanied by the high local field enhancement (~10(3)) characteristic of a nano-antenna type pattern. Rigorous numerical simulations of the field distribution are presented to explain the different observed phenomena.
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spelling pubmed-66512482019-08-07 Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor Isaacs, Sivan Hajoj, Ansar Abutoama, Mohammad Kozlovsky, Alexander Golan, Erez Abdulhalim, Ibrahim Sensors (Basel) Article Dielectric grating-based sensors are usually based on the guided mode resonance (GMR) obtained using a thin planar waveguide layer (PWL) adjacent to a thin subwavelength grating layer. In this work, we present a detailed investigation of thick subwavelength dielectric grating structures that exhibit reflection resonances above a certain thickness without the need for the waveguide layer, showing great potential for applications in biosensing and tunable filtering. Analytic and numerical results are thoroughly discussed, as well as an experimental demonstration of the structure as a chemical sensor in the SWIR (short wave infrared) spectral range (1200–1800 nm). In comparison to the GMR structure with PWL, the thick grating structure has several unique properties: (i) It gives higher sensitivity when the spaces are filled, with the analyte peaking at certain space values due to an increase in the interaction volume between the analyte and the evanescent optical field between the grating lines; (ii) the TM (transverse magnetic) resonance, in certain cases, provides a better figure of merit; (iii) the sensitivity increases as the grating height increases; (iv) the prediction of the resonance locations based on the effective medium approximation does not give satisfactory results when the grating height is larger than a certain value, and the invalidity becomes more severe as the period increases; (v) a sudden increase in the Q-factor of the resonance occurs at a specific height value accompanied by the high local field enhancement (~10(3)) characteristic of a nano-antenna type pattern. Rigorous numerical simulations of the field distribution are presented to explain the different observed phenomena. MDPI 2019-07-08 /pmc/articles/PMC6651248/ /pubmed/31288404 http://dx.doi.org/10.3390/s19133003 Text en © 2019 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 (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Isaacs, Sivan
Hajoj, Ansar
Abutoama, Mohammad
Kozlovsky, Alexander
Golan, Erez
Abdulhalim, Ibrahim
Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title_full Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title_fullStr Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title_full_unstemmed Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title_short Resonant Grating without a Planar Waveguide Layer as a Refractive Index Sensor
title_sort resonant grating without a planar waveguide layer as a refractive index sensor
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6651248/
https://www.ncbi.nlm.nih.gov/pubmed/31288404
http://dx.doi.org/10.3390/s19133003
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