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Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers?
The study presents a novel demonstration of a passively mode-locked erbium-doped fiber laser (EDFL) that is based on a silicon carbide (Si(x)C(1−x)) saturable absorber. When the C/Si composition ratio is increased to 1.83, the Si(x)C(1−x) film transforms from two-photon absorption to nonlinear satur...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4642298/ https://www.ncbi.nlm.nih.gov/pubmed/26558531 http://dx.doi.org/10.1038/srep16463 |
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author | Cheng, Chih-Hsien Lin, Yung-Hsiang Chen, Ting-Hui Chen, Hsiang-Yu Chi, Yu-Chieh Leeb, Chao-Kuei Wua, Chih-I Lin, Gong-Ru |
author_facet | Cheng, Chih-Hsien Lin, Yung-Hsiang Chen, Ting-Hui Chen, Hsiang-Yu Chi, Yu-Chieh Leeb, Chao-Kuei Wua, Chih-I Lin, Gong-Ru |
author_sort | Cheng, Chih-Hsien |
collection | PubMed |
description | The study presents a novel demonstration of a passively mode-locked erbium-doped fiber laser (EDFL) that is based on a silicon carbide (Si(x)C(1−x)) saturable absorber. When the C/Si composition ratio is increased to 1.83, the Si(x)C(1−x) film transforms from two-photon absorption to nonlinear saturable absorption, and the corresponding value reaches −3.9 × 10(−6) cm/W. The Si-rich Si(x)C(1−x) film cannot mode lock the EDFL because it induced high intracavity loss through two-photon absorption. Even when a stoichiometric SiC is used, the EDFL is mode locked, similar to an EDFL operating under weak nonlinear-polarization-rotation condition. A C-rich Si(x)C(1−x) film containing sp(2)-orbital C–C bonds with a linear absorbance of 0.172 and nonlinear absorbance of 0.04 at a 181 MW/cm(2) saturation intensity demonstrates nonlinear transmittance. The C-rich Si(x)C(1−x) saturable absorber successfully generates a short mode-locked EDFL pulse of 470 fs. The fluctuation of the pulse-train envelope dropps considerably from 11.6% to 0.8% when a strong saturable-absorption-induced self-amplitude modulation process occurs in the C-rich Si(x)C(1−x) film. |
format | Online Article Text |
id | pubmed-4642298 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-46422982015-11-20 Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? Cheng, Chih-Hsien Lin, Yung-Hsiang Chen, Ting-Hui Chen, Hsiang-Yu Chi, Yu-Chieh Leeb, Chao-Kuei Wua, Chih-I Lin, Gong-Ru Sci Rep Article The study presents a novel demonstration of a passively mode-locked erbium-doped fiber laser (EDFL) that is based on a silicon carbide (Si(x)C(1−x)) saturable absorber. When the C/Si composition ratio is increased to 1.83, the Si(x)C(1−x) film transforms from two-photon absorption to nonlinear saturable absorption, and the corresponding value reaches −3.9 × 10(−6) cm/W. The Si-rich Si(x)C(1−x) film cannot mode lock the EDFL because it induced high intracavity loss through two-photon absorption. Even when a stoichiometric SiC is used, the EDFL is mode locked, similar to an EDFL operating under weak nonlinear-polarization-rotation condition. A C-rich Si(x)C(1−x) film containing sp(2)-orbital C–C bonds with a linear absorbance of 0.172 and nonlinear absorbance of 0.04 at a 181 MW/cm(2) saturation intensity demonstrates nonlinear transmittance. The C-rich Si(x)C(1−x) saturable absorber successfully generates a short mode-locked EDFL pulse of 470 fs. The fluctuation of the pulse-train envelope dropps considerably from 11.6% to 0.8% when a strong saturable-absorption-induced self-amplitude modulation process occurs in the C-rich Si(x)C(1−x) film. Nature Publishing Group 2015-11-12 /pmc/articles/PMC4642298/ /pubmed/26558531 http://dx.doi.org/10.1038/srep16463 Text en Copyright © 2015, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Cheng, Chih-Hsien Lin, Yung-Hsiang Chen, Ting-Hui Chen, Hsiang-Yu Chi, Yu-Chieh Leeb, Chao-Kuei Wua, Chih-I Lin, Gong-Ru Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title | Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title_full | Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title_fullStr | Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title_full_unstemmed | Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title_short | Can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
title_sort | can silicon carbide serve as a saturable absorber for passive mode-locked fiber lasers? |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4642298/ https://www.ncbi.nlm.nih.gov/pubmed/26558531 http://dx.doi.org/10.1038/srep16463 |
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