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Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering

Fano resonance, known for its unique asymmetric line shape, has gained significant attention in photonics, particularly in sensing applications. However, it remains difficult to achieve controllable Fano parameters with a simple geometric structure. Here, a novel approach of using a thin‐film optica...

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Autores principales: Ko, Joo Hwan, Park, Jin‐Hwi, Yoo, Young Jin, Chang, Sehui, Kang, Jiwon, Wu, Aiguo, Yang, Fang, Kim, Sejeong, Jeon, Hae‐Gon, Song, Young Min
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10646235/
https://www.ncbi.nlm.nih.gov/pubmed/37691086
http://dx.doi.org/10.1002/advs.202304310
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author Ko, Joo Hwan
Park, Jin‐Hwi
Yoo, Young Jin
Chang, Sehui
Kang, Jiwon
Wu, Aiguo
Yang, Fang
Kim, Sejeong
Jeon, Hae‐Gon
Song, Young Min
author_facet Ko, Joo Hwan
Park, Jin‐Hwi
Yoo, Young Jin
Chang, Sehui
Kang, Jiwon
Wu, Aiguo
Yang, Fang
Kim, Sejeong
Jeon, Hae‐Gon
Song, Young Min
author_sort Ko, Joo Hwan
collection PubMed
description Fano resonance, known for its unique asymmetric line shape, has gained significant attention in photonics, particularly in sensing applications. However, it remains difficult to achieve controllable Fano parameters with a simple geometric structure. Here, a novel approach of using a thin‐film optical Fano resonator with a porous layer to generate entire spectral shapes from quasi‐Lorentzian to Lorentzian to Fano is proposed and experimentally demonstrated. The glancing angle deposition technique is utilized to create a polarization‐dependent Fano resonator. By altering the linear polarization between s‐ and p‐polarization, a switchable Fano device between quasi‐Lorentz state and negative Fano state is demonstrated. This change in spectral shape is advantageous for detecting materials with a low‐refractive index. A bio‐particle sensing experiment is conducted that demonstrates an enhanced signal‐to‐noise ratio and prediction accuracy. Finally, the challenge of optimizing the film‐based Fano resonator due to intricate interplay among numerous parameters, including layer thicknesses, porosity, and materials selection, is addressed. The inverse design tool is developed based on a multilayer perceptron model that allows fast computation for all ranges of Fano parameters. The method provides improved accuracy of the mean validation factor (MVF = 0.07, q‐q') compared to the conventional exhaustive enumeration method (MVF = 0.37).
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spelling pubmed-106462352023-09-10 Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering Ko, Joo Hwan Park, Jin‐Hwi Yoo, Young Jin Chang, Sehui Kang, Jiwon Wu, Aiguo Yang, Fang Kim, Sejeong Jeon, Hae‐Gon Song, Young Min Adv Sci (Weinh) Research Article Fano resonance, known for its unique asymmetric line shape, has gained significant attention in photonics, particularly in sensing applications. However, it remains difficult to achieve controllable Fano parameters with a simple geometric structure. Here, a novel approach of using a thin‐film optical Fano resonator with a porous layer to generate entire spectral shapes from quasi‐Lorentzian to Lorentzian to Fano is proposed and experimentally demonstrated. The glancing angle deposition technique is utilized to create a polarization‐dependent Fano resonator. By altering the linear polarization between s‐ and p‐polarization, a switchable Fano device between quasi‐Lorentz state and negative Fano state is demonstrated. This change in spectral shape is advantageous for detecting materials with a low‐refractive index. A bio‐particle sensing experiment is conducted that demonstrates an enhanced signal‐to‐noise ratio and prediction accuracy. Finally, the challenge of optimizing the film‐based Fano resonator due to intricate interplay among numerous parameters, including layer thicknesses, porosity, and materials selection, is addressed. The inverse design tool is developed based on a multilayer perceptron model that allows fast computation for all ranges of Fano parameters. The method provides improved accuracy of the mean validation factor (MVF = 0.07, q‐q') compared to the conventional exhaustive enumeration method (MVF = 0.37). John Wiley and Sons Inc. 2023-09-10 /pmc/articles/PMC10646235/ /pubmed/37691086 http://dx.doi.org/10.1002/advs.202304310 Text en © 2023 The Authors. Advanced Science published by Wiley‐VCH GmbH https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Research Article
Ko, Joo Hwan
Park, Jin‐Hwi
Yoo, Young Jin
Chang, Sehui
Kang, Jiwon
Wu, Aiguo
Yang, Fang
Kim, Sejeong
Jeon, Hae‐Gon
Song, Young Min
Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title_full Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title_fullStr Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title_full_unstemmed Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title_short Full‐Control and Switching of Optical Fano Resonance by Continuum State Engineering
title_sort full‐control and switching of optical fano resonance by continuum state engineering
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10646235/
https://www.ncbi.nlm.nih.gov/pubmed/37691086
http://dx.doi.org/10.1002/advs.202304310
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