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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...

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Detalles Bibliográficos
Autores principales: Cheng, Chih-Hsien, Lin, Yung-Hsiang, Chen, Ting-Hui, Chen, Hsiang-Yu, Chi, Yu-Chieh, Leeb, Chao-Kuei, Wua, Chih-I, Lin, Gong-Ru
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
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
Descripción
Sumario: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.