• Title/Summary/Keyword: Nonlinear polarization rotation

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Regenerative Er-doped Fiber Amplifier System for High-repetition-rate Optical Pulses

  • Liu, Yan;Wu, Kan;Li, Nanxi;Lan, Lanling;Yoo, Seongwoo;Wu, Xuan;Shum, Perry Ping;Zeng, Shuguang;Tan, Xinyu
    • Journal of the Optical Society of Korea
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    • v.17 no.5
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    • pp.357-361
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    • 2013
  • A regenerative Er-doped fiber amplifier system for a high-repetition-rate optical pulse train is investigated for the first time. A signal pulse train with a wavelength tuning range of 18 nm is produced by a passive mode-locked fiber laser based on a nonlinear polarization rotation technique. In order to realize the amplification, an optical delay-line is used to achieve time match between the pulses' interval and the period of pulse running through the regenerative amplifier. The 16 dB gain is obtained for an input pulse train with a launching power of -30.4 dBm, a center wavelength of 1563.4 nm and a repetition rate of 15.3 MHz. The output properties of signal pulses with different center wavelengths are also discussed. The pulse amplification is found to be different from the regenerative amplification system for CW signals.

Passively Mode-Locked 1.93-㎛ All-Fiberized Femtosecond MOPA Laser Using a Gold-Deposited Side-Polished Fiber (금 증착 측면연마 광섬유를 이용한 1.93㎛ 모드잠금 펨토초 전광섬유 MOPA 레이저)

  • Jung, Minwan;Koo, Joonhoi;Lee, Ju Han
    • Korean Journal of Optics and Photonics
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    • v.25 no.6
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    • pp.340-345
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    • 2014
  • We experimentally demonstrate the use of a gold-deposited side-polished fiber as a $2-{\mu}m$-band polarizing device to produce mode-locked pulses from a thulium/holmium-codoped fiber ring cavity. The mode-locking effect was induced by nonlinear transmission caused by the gold-deposited side-polished fiber, due to nonlinear polarization rotation of the oscillated beam within the fiberized cavity. It is also shown that ~558-fs pulses with a peak power of ~6.7 kW could readily be produced at a wavelength of 1935 nm through subsequent thulium/holmium-codoped fiber amplification, due to the higher-order soliton compression effect.