4.7 Article

Intracavity Tandemly-Pumped and Gain-Switched Tm-doped Fiber Laser at 1.7 μm

Journal

JOURNAL OF LIGHTWAVE TECHNOLOGY
Volume 40, Issue 13, Pages 4373-4378

Publisher

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/JLT.2022.3158316

Keywords

Pump lasers; Laser excitation; Laser modes; Erbium-doped fiber lasers; Power lasers; Optical fiber devices; Mathematical models; Fiber lasers; pulsed lasers; short wavelength; thulium-doped fiber

Funding

  1. National Natural Science Foundation of China [62075159, 61975146]
  2. Major Scientific and Technological Innovation Projects of Key R&D Plans in Shandong Province [2019JZZY020206]

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In this study, a novel method was proposed and demonstrated to achieve pulsed operation of thulium-doped fiber lasers at 1.7 μm. By embedding the thulium-doped fiber laser cavity within the cavity of an erbium/ytterbium-codoped fiber laser operating at 1.5 μm, the 1.5 μm laser was forced to operate in a passively Q-switched scheme using the thulium-doped fiber as a saturable absorber. The thulium-doped fiber laser at 1.7 μm was then pumped by the Q-switched 1.5 μm laser and gain-switched. The experimental results matched well with the theoretical model, providing insights for further improving the laser performance.
We propose and demonstrate a novel method to achieve pulsed operation of thulium-doped fiber lasers at 1.7 mu m. In our design, the thulium-doped fiber laser cavity was embedded within the cavity of an erbium/ytterbium-codoped fiber laser operating at 1.5 mu m. The thulium-doped fiber in the erbium/ytterbium-codoped fiber laser cavity served as a saturable absorber, forcing the 1.5 mu m laser to operate in a passively Q-switched scheme. The 1.7 mu m thulium-doped fiber laser was in-turn pumped by the Q-switched 1.5 mu m laser and was gain-switched. This made the pulse duration of 1.7 mu m emission much shorter than that of 1.5 mu m emission. 1.02 W average output power at 1720 nm was obtained for 10 W of pump power at 976 nm. The pulse repetition frequency, pulse energy and pulse duration were 134 kHz, 7.6 mu J and 102 ns, respectively. A rate equation model was developed to examine the power- and temporal-behavior of the laser system. The calculated pulse duration and pulse repetition frequency matched well with the experimental results. Methods of further improving the laser performance are discussed based on insights gleaned from our modeling.

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