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Numerical model for enhancing stimulated Brillouin scattering in optical microfibers
Stimulated Brillouin scattering (SBS) is useful, among others for generating slow light, sensing and amplification. SBS was previously viewed as a poor method due to the limitation on optical power in high-powered photonic applications. However, considering the many possible applications using SBS,...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
F1000 Research Limited
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10517297/ https://www.ncbi.nlm.nih.gov/pubmed/37745939 http://dx.doi.org/10.12688/f1000research.51029.2 |
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author | Yeap, Soon Heng Emami, Siamak Dawazdah Abdul-Rashid, Hairul Azhar |
author_facet | Yeap, Soon Heng Emami, Siamak Dawazdah Abdul-Rashid, Hairul Azhar |
author_sort | Yeap, Soon Heng |
collection | PubMed |
description | Stimulated Brillouin scattering (SBS) is useful, among others for generating slow light, sensing and amplification. SBS was previously viewed as a poor method due to the limitation on optical power in high-powered photonic applications. However, considering the many possible applications using SBS, it is now of interest to enhance SBS in areas of Brillouin frequency shift together with Brillouin Gain. A numerical model, using a fully vectorial approach, by employing the finite element method, was developed to investigate methods for enhancing SBS in optical fiber. This paper describes the method related to the numerical model and discusses the analysis between the interactions of longitudinal, shear and hybrid acoustic modes; and optical modes in optical fiber. Two case studies were used to demonstrate this. Based on this numerical model, we report the influence of core radius, clad radius and effective refractive index on the Brillouin frequency shift and gain. We observe the difference of Brillouin shift frequency between a normal silica optical fiber and that of a microfiber - a uniformed silica fiber of a much smaller core and cladding dimensions where nonlinearities are higher. Also observed, the different core radii used and their respective Brillouin shift. For future work, the COMSOL model can also be used for the following areas of research, including simulating “surface Brillouin shift” and also to provide in-sights to the Brillouin shift frequency vB of various structures of waveguides, e.g circular, and triangular, and also to examine specialty fibers, e.g. Thulium and Chalcogenide doped fibers, and their effects on Brillouin shift frequency. |
format | Online Article Text |
id | pubmed-10517297 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | F1000 Research Limited |
record_format | MEDLINE/PubMed |
spelling | pubmed-105172972023-09-24 Numerical model for enhancing stimulated Brillouin scattering in optical microfibers Yeap, Soon Heng Emami, Siamak Dawazdah Abdul-Rashid, Hairul Azhar F1000Res Method Article Stimulated Brillouin scattering (SBS) is useful, among others for generating slow light, sensing and amplification. SBS was previously viewed as a poor method due to the limitation on optical power in high-powered photonic applications. However, considering the many possible applications using SBS, it is now of interest to enhance SBS in areas of Brillouin frequency shift together with Brillouin Gain. A numerical model, using a fully vectorial approach, by employing the finite element method, was developed to investigate methods for enhancing SBS in optical fiber. This paper describes the method related to the numerical model and discusses the analysis between the interactions of longitudinal, shear and hybrid acoustic modes; and optical modes in optical fiber. Two case studies were used to demonstrate this. Based on this numerical model, we report the influence of core radius, clad radius and effective refractive index on the Brillouin frequency shift and gain. We observe the difference of Brillouin shift frequency between a normal silica optical fiber and that of a microfiber - a uniformed silica fiber of a much smaller core and cladding dimensions where nonlinearities are higher. Also observed, the different core radii used and their respective Brillouin shift. For future work, the COMSOL model can also be used for the following areas of research, including simulating “surface Brillouin shift” and also to provide in-sights to the Brillouin shift frequency vB of various structures of waveguides, e.g circular, and triangular, and also to examine specialty fibers, e.g. Thulium and Chalcogenide doped fibers, and their effects on Brillouin shift frequency. F1000 Research Limited 2022-02-17 /pmc/articles/PMC10517297/ /pubmed/37745939 http://dx.doi.org/10.12688/f1000research.51029.2 Text en Copyright: © 2022 Yeap SH et al. https://creativecommons.org/licenses/by/4.0/This is an open access article distributed under the terms of the Creative Commons Attribution Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. |
spellingShingle | Method Article Yeap, Soon Heng Emami, Siamak Dawazdah Abdul-Rashid, Hairul Azhar Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title | Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title_full | Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title_fullStr | Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title_full_unstemmed | Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title_short | Numerical model for enhancing stimulated Brillouin scattering in optical microfibers |
title_sort | numerical model for enhancing stimulated brillouin scattering in optical microfibers |
topic | Method Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10517297/ https://www.ncbi.nlm.nih.gov/pubmed/37745939 http://dx.doi.org/10.12688/f1000research.51029.2 |
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