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Compact fs ytterbium fiber laser at 1010 nm for biomedical applications.
Kong, Cihang; Pilger, Christian; Hachmeister, Henning; Wei, Xiaoming; Cheung, Tom H; Lai, Cora S W; Huser, Thomas; Tsia, Kevin K; Wong, Kenneth K Y.
Afiliação
  • Kong C; Electrical and Electronic Engineering, The University of Hong Kong, Pokfulam Road, Hong Kong, China.
  • Pilger C; These authors contributed equally to the paper.
  • Hachmeister H; Biomolecular Photonics, Department of Physics, University of Bielefeld, Universitätsstr, 25, 33615 Bielefeld, Germany.
  • Wei X; These authors contributed equally to the paper.
  • Cheung TH; Biomolecular Photonics, Department of Physics, University of Bielefeld, Universitätsstr, 25, 33615 Bielefeld, Germany.
  • Lai CSW; These authors contributed equally to the paper.
  • Huser T; Electrical and Electronic Engineering, The University of Hong Kong, Pokfulam Road, Hong Kong, China.
  • Tsia KK; xmwei@eee.hku.hk.
  • Wong KKY; Division of Life Science, The Hong Kong University of Science and Technology, Hong Kong, China.
Biomed Opt Express ; 8(11): 4921-4932, 2017 Nov 01.
Article em En | MEDLINE | ID: mdl-29188091
ABSTRACT
Ytterbium-doped fiber lasers (YDFLs) working in the near-infrared (NIR) spectral window and capable of high-power operation are popular in recent years. They have been broadly used in a variety of scientific and industrial research areas, including light bullet generation, optical frequency comb formation, materials fabrication, free-space laser communication, and biomedical diagnostics as well. The growing interest in YDFLs has also been cultivated for the generation of high-power femtosecond (fs) pulses. Unfortunately, the operating wavelengths of fs YDFLs have mostly been confined to two spectral bands, i.e., 970-980 nm through the three-level energy transition and 1030-1100 nm through the quasi three-level energy transition, leading to a spectral gap (990-1020 nm) in between, which is attributed to an intrinsically weak gain in this wavelength range. Here we demonstrate a high-power mode-locked fs YDFL operating at 1010 nm, which is accomplished in a compact and cost-effective package. It exhibits superior performance in terms of both short-term and long-term stability, i.e., <0.3% (peak intensity over 2.4 µs) and <4.0% (average power over 24 hours), respectively. To illustrate the practical applications, it is subsequently employed as a versatile fs laser for high-quality nonlinear imaging of biological samples, including two-photon excited fluorescence microscopy of mouse kidney and brain sections, as well as polarization-sensitive second-harmonic generation microscopy of potato starch granules and mouse tail muscle. It is anticipated that these efforts will largely extend the capability of fs YDFLs which is continuously tunable over 970-1100 nm wavelength range for wideband hyperspectral operations, serving as a promising complement to the gold-standard Tisapphire fs lasers.
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Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article