Abstract

We report a gain-switched diode-seeded thulium doped fiber master oscillator power amplifier (MOPA) producing up to 295-kW picosecond pulses (35 ps) at a repetition rate of 1 MHz with a good beam quality (M2 ~1.3). A narrow-band, grating-based filter was incorporated within the amplifier chain to restrict the accumulation of nonlinear spectral broadening and counter-pumping of a short length of large-mode-area (LMA) fiber was used in the final stage amplifier to further reduce nonlinear effects. Finally, we generated watt-level >2.5-octave supercontinuum spanning from 750 nm to 5000 nm by using the MOPA output to pump an indium fluoride fiber.

Highlights

  • Thulium doped fiber lasers (TDFLs) have experienced rapid development in the past few years, driven by a diverse range of applications including gas sensing, laser processing of both polymers and biological tissues, and nonlinear frequency conversion [1,2,3,4,5]

  • We report a gain-switched diode-seeded thulium doped fiber master oscillator power amplifier (MOPA) producing up to 295-kW picosecond pulses (35 ps) at a repetition rate of 1 MHz with a good beam quality (M2 ~1.3)

  • Funding EPSRC AirGuide Photonics Programme Grant (Grant EP/P030181/1) Acknowledgment The authors acknowledge Dr Peter Shardlow from ORC for providing the in-house fabricated thulium doped fibers

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Summary

Introduction

Thulium doped fiber lasers (TDFLs) have experienced rapid development in the past few years, driven by a diverse range of applications including gas sensing, laser processing of both polymers and biological tissues, and nonlinear frequency conversion [1,2,3,4,5]. Wang et al recently presented a nanosecond-pulsed thulium-doped LMA-fiber MOPA system with an average output power scalable from 150 W to 238 W [9]. Stutzki et al reported femtosecond pulses with a peak power in excess of 200 MW from a CPA system based on a LMA thulium doped fiber with 25-μm core diameter and a thulium-doped large-pitch rod fiber with a mode field diameter of 65 μm, respectively [14,15]. High-power picosecond lasers can be a good option for many nonlinear frequency conversion applications due to the simpler system architectures compared to femtosecond CPA systems and much shorter pulse duration in comparison to nanosecond lasers [16]. Careful management of fiber nonlinearity and signal purity are essential to accomplish further power scaling from thulium-doped fiber MOPA systems

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