Abstract

Abstract In this paper, an all-fiberized and narrow-linewidth 5 kW power-level fiber amplifier is presented. The laser is achieved based on the master oscillator power amplification configuration, in which the phase-modulated single-frequency laser is applied as the seed laser and a bidirectional pumping configuration is applied in the power amplifier. The stimulated Brillouin scattering, stimulated Raman scattering, and transverse mode instability effects are all effectively suppressed in the experiment. Consequently, the output power is scaled up to 4.92 kW with a slope efficiency of as high as approximately 80%. The 3-dB spectral width is about 0.59 nm, and the beam quality is measured to be M2∼1.22 at maximum output power. Furthermore, we have also conducted a detailed spectral analysis on the spectral width of the signal laser, which reveals that the spectral wing broadening phenomenon could lead to the obvious decrease of the spectral purity at certain output power. Overall, this work could provide a reference for obtaining and optimizing high-power narrow-linewidth fiber lasers.

Highlights

  • High-power narrow-linewidth fiber lasers with excellent beam quality have been highly desired for spectral and coherent beam combinations[1,2,3]

  • To ensure sufficient enhancement of the stimulated Brillouin scattering (SBS) threshold, a filtered white noise signal (WNS) with electronic bandwidth of 12 GHz and RF power of 0.26 W is applied to the electro-optic modulator (EOM) for phase modulation and spectral broadening

  • The spectrum of the signal laser is measured through a commercial optical spectral analyzer (OSA) with the spectral resolution of 0.02 nm here and in the following experiments

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Summary

Introduction

High-power narrow-linewidth fiber lasers with excellent beam quality have been highly desired for spectral and coherent beam combinations[1,2,3]. The power scaling of single-mode narrow-linewidth fiber lasers has been under intense investigation[4,5,6,7,8,9,10,11,12,13,14,15]. This mainly involves comprehensive suppressions of the transverse mode instabilities (TMIs) and nonlinear inelastic scattering effects, such as stimulated Brillouin scattering (SBS) and stimulated Raman scattering (SRS)[16,17,18]. The SBS/SRS effects could be suppressed through reducing the effective fiber length

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