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Deep-ultraviolet second-harmonic generation by combined degenerate four-wave mixing and surface nonlinearity polarization in photonic crystal fiber

Deep-ultraviolet (UV) second-harmonics (SHs) have important applications in basic physics and applied sciences. However, it still remains challenging to generate deep-UV SHs especially in optical fibers. Here, for the first time, we experimentally demonstrate the deep-UV SH generations (SHGs) by com...

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Detalles Bibliográficos
Autores principales: Yuan, Jinhui, Kang, Zhe, Li, Feng, Zhou, Guiyao, Zhang, Xianting, Mei, Chao, Sang, Xinzhu, Wu, Qiang, Yan, Binbin, Zhou, Xian, Zhong, Kangping, Wang, Kuiru, Yu, Chongxiu, Lu, Chao, Tam, Hwa Yaw, Wai, P. K. A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5569049/
https://www.ncbi.nlm.nih.gov/pubmed/28835701
http://dx.doi.org/10.1038/s41598-017-10028-3
Descripción
Sumario:Deep-ultraviolet (UV) second-harmonics (SHs) have important applications in basic physics and applied sciences. However, it still remains challenging to generate deep-UV SHs especially in optical fibers. Here, for the first time, we experimentally demonstrate the deep-UV SH generations (SHGs) by combined degenerate four-wave mixing (FWM) and surface nonlinearity polarization in an in-house designed and fabricated air-silica photonic crystal fiber (PCF). When femtosecond pump pulses with average input power P (av) of 650 mW and center wavelength λ (p) of 810, 820, 830, and 840 nm are coupled into the normal dispersion region close to the zero-dispersion wavelength of the fundamental mode of the PCF, the anti-Stokes waves induced by degenerate FWM process are tunable from 669 to 612 nm. Then, they serve as the secondary pump, and deep-UV SHs are generated within the wavelength range of 334.5 to 306 nm as a result of surface nonlinearity polarization at the core-cladding interface of the PCF. The physical mechanism of the SHGs is confirmed by studying the dependences of the output power P (SH) of the SHs on the PCF length and time. Finally, we also establish a theoretical model to analyze the SHGs.