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Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances

Wideband excitation and control of Fano resonance and electromagnetically induced transparency (EIT), both of which rely on coherent interaction between two excitation paths, is challenging. It requires precise control and tuning of interacting resonances or coupling between different resonant struc...

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Autores principales: Pant, Ravi, A., Siva Shakthi, Yelikar, Anjali B.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6003991/
https://www.ncbi.nlm.nih.gov/pubmed/29907792
http://dx.doi.org/10.1038/s41598-018-27444-8
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author Pant, Ravi
A., Siva Shakthi
Yelikar, Anjali B.
author_facet Pant, Ravi
A., Siva Shakthi
Yelikar, Anjali B.
author_sort Pant, Ravi
collection PubMed
description Wideband excitation and control of Fano resonance and electromagnetically induced transparency (EIT), both of which rely on coherent interaction between two excitation paths, is challenging. It requires precise control and tuning of interacting resonances or coupling between different resonant structures over a wide frequency range. Gain (Stokes) and absorption (anti-Stokes) resonances associated with the stimulated Brillouin scattering (SBS) process can be excited and controlled over a wide frequency range by tuning the pump frequency, its power and profile. We exploit coherent interaction between the Brillouin Stokes and anti-Stokes resonance, in radio frequency domain, to demonstrate Fano and EIT-like resonance over a wide frequency range and control their shape and strength optically and electrically. For the Fano resonance, the asymmetry and polarity are electrically controlled over an unprecedented frequency range (100 MHz–43 GHz) by varying the bias to the intensity modulator whereas, the strength is varied by tuning the Brillouin pump power and/or the bias. The depth and 3 dB linewidth of the transparency window in the EIT-like resonance are controlled using pump and probe parameters. The flexibility of the SBS process that allows wideband electrical and optical control of Fano and EIT-like resonance opens up the potential for applications that range from low-power switching, sensing to tunable RF delay.
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spelling pubmed-60039912018-06-26 Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances Pant, Ravi A., Siva Shakthi Yelikar, Anjali B. Sci Rep Article Wideband excitation and control of Fano resonance and electromagnetically induced transparency (EIT), both of which rely on coherent interaction between two excitation paths, is challenging. It requires precise control and tuning of interacting resonances or coupling between different resonant structures over a wide frequency range. Gain (Stokes) and absorption (anti-Stokes) resonances associated with the stimulated Brillouin scattering (SBS) process can be excited and controlled over a wide frequency range by tuning the pump frequency, its power and profile. We exploit coherent interaction between the Brillouin Stokes and anti-Stokes resonance, in radio frequency domain, to demonstrate Fano and EIT-like resonance over a wide frequency range and control their shape and strength optically and electrically. For the Fano resonance, the asymmetry and polarity are electrically controlled over an unprecedented frequency range (100 MHz–43 GHz) by varying the bias to the intensity modulator whereas, the strength is varied by tuning the Brillouin pump power and/or the bias. The depth and 3 dB linewidth of the transparency window in the EIT-like resonance are controlled using pump and probe parameters. The flexibility of the SBS process that allows wideband electrical and optical control of Fano and EIT-like resonance opens up the potential for applications that range from low-power switching, sensing to tunable RF delay. Nature Publishing Group UK 2018-06-15 /pmc/articles/PMC6003991/ /pubmed/29907792 http://dx.doi.org/10.1038/s41598-018-27444-8 Text en © The Author(s) 2018 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
Pant, Ravi
A., Siva Shakthi
Yelikar, Anjali B.
Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title_full Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title_fullStr Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title_full_unstemmed Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title_short Wideband excitation of Fano resonances and induced transparency by coherent interactions between Brillouin resonances
title_sort wideband excitation of fano resonances and induced transparency by coherent interactions between brillouin resonances
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6003991/
https://www.ncbi.nlm.nih.gov/pubmed/29907792
http://dx.doi.org/10.1038/s41598-018-27444-8
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