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5.1 kW Tandem-Pumped Fiber Amplifier Seeded by Random Fiber Laser With High Suppression of Stimulated Raman Scattering | IEEE Journals & Magazine | IEEE Xplore

5.1 kW Tandem-Pumped Fiber Amplifier Seeded by Random Fiber Laser With High Suppression of Stimulated Raman Scattering


Impact Statement:A monolithic high-power tandem-pumped random fiber laser with a great SRS suppression is built successfully. 1) The output Power reaches 5.1 kW, which is the highest repo...Show More

Abstract:

In this work, high-power tandem-pumped random fiber lasers are investigated in detail. A 6.5 W random fiber laser seed centered at 1070 nm with a half-open cavity structu...Show More
Impact Statement:
A monolithic high-power tandem-pumped random fiber laser with a great SRS suppression is built successfully. 1) The output Power reaches 5.1 kW, which is the highest report in random fiber laser. 2) The total optical-to-optical efficiency is 89.0%, which is the highest report in random fiber laser in kilowatts level. 3) To suppress the SRS effect, several methods are applied including avoiding external feedback, adopting high core/clad diameter ratio fiber and using a BPF to mitigate Raman noise. SRS suppression ratio reaches 27 dB at 5.1 kW.

Abstract:

In this work, high-power tandem-pumped random fiber lasers are investigated in detail. A 6.5 W random fiber laser seed centered at 1070 nm with a half-open cavity structure was built. Boosted by two amplifier stages, the random fiber laser achieved a power of several kilowatts. Stimulated Raman scattering (SRS) mitigation is challenging in tandem-pumped fiber lasers. To suppress SRS, several methods were applied, including avoiding external feedback in the oscillator stage, incorporating a high core/cladding diameter ratio gain fiber, and using a band pass filter (BPF) to mitigate Raman noise. The latter proved to be the most effective method; therefore, SRS mitigation without and with a BPF was investigated at 3.5 kW, leading to suppression ratios rising from 14 to 30 dB. By increasing the pump power continuously to 5.6 kW, we realized a record output power of 5.1 kW, corresponding to an SRS suppression ratio of 27 dB. Owing to the high-brightness 1018 nm fiber lasers serving as the p...
Published in: IEEE Journal of Quantum Electronics ( Volume: 57, Issue: 2, April 2021)
Article Sequence Number: 6800109
Date of Publication: 30 December 2020

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I. Introduction

Since their inception toward the end of the 20th century, random lasers, via multiple scattering in a disordered gain medium, have shown some intriguing properties that distinguish them from traditional fixed cavity structure lasers [1]–[3]. However, limited by low output power and poor directivity, random lasers are very difficult to apply practically. In the past decade, a novel one-dimensional random laser utilizing optical fiber as the medium has been proposed and studied in depth [4]–[7]. The random Raman fiber laser (RRFL) is based on Rayleigh scattering and amplified by stimulated Raman scattering (SRS). The waveguide structure of the fiber restricts scattering in the radial direction, leading to greatly enhanced directivity and a relatively low laser threshold, which makes RRFLs more applicable than other random laser designs.

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