Invited Paper: High-power monolithic narrow-linewidth 1.6 mJ/8 ns fiber laser system based on all-glass spun tapered double-clad fiber amplifier

High-energy, narrow-linewidth nanosecond pulses are highly demanding for many applications that require high temporal and spatial coherence. However, the amplification of narrow-linewidth pulses is primarily limited by stimulated Brillouin scattering, which causes pulse instabilities, back-reflected pulses, and catastrophic damage effects on optical components. In this work, we present a 1.6 mJ narrow-linewidth nanosecond pulsed fiber laser system based on all-glass spun tapered double-clad fibers without employing any mitigating technique for the stimulated Brillouin scattering effect. The system delivers pulses with an 8 ns duration at a 100 kHz repetition rate, over 97.5% degree of polarization, a beam quality factor of M 2 ∼ 1 . 3 , a spectral linewidth of 53.8 MHz, a 160 W average power, and 188 kW peak power with a slope efficiency of 97.6%. The degree of spatial coherence of the amplified signal was measured to be 0.94. Our results are highly valued in applications requiring high-energy, high-coherence pulses with spectral, spatial, and polarization characteristics in a compact system. • High energy/high peak power nanosecond pulsed fiber-based laser system with near-diffraction-limited beam quality. • High temporal and spatial coherence. • Efficient SBS suppression by a spun tapered double-clad fiber. • Compact, stable, all-fiber monolithic system ideal for field application.

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Publication Details

Journal
Optical Fiber Technology
Published
2025-11-20
DOI
https://doi.org/10.1016/j.yofte.2025.104465
Citations
2
Primary Topic
Photonic Crystal and Fiber Optics
Type
article
Field-Weighted Citation Impact
1.46
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article

Invited Paper: High-power monolithic narrow-linewidth 1.6 mJ/8 ns fiber laser system based on all-glass spun tapered double-clad fiber amplifier

Evgenii A. Motorin, Regina Gumenyuk, Ebrahim Aghayari, Matias Koivurova et al.
2 citations
Optical Fiber Technology
Photonic Crystal and Fiber Optics
1.46
article

Invited Paper: High-power monolithic narrow-linewidth 1.6 mJ/8 ns fiber laser system based on all-glass spun tapered double-clad fiber amplifier

Evgenii A. Motorin, Regina Gumenyuk, Ebrahim Aghayari, Matias Koivurova, Hossein Fathi, Uttam Kumar Samanta, В. Н. Филиппов, Andrey Grishchenko
article en
2 citations

Abstract

High-energy, narrow-linewidth nanosecond pulses are highly demanding for many applications that require high temporal and spatial coherence. However, the amplification of narrow-linewidth pulses is primarily limited by stimulated Brillouin scattering, which causes pulse instabilities, back-reflected pulses, and catastrophic damage effects on optical components. In this work, we present a 1.6 mJ narrow-linewidth nanosecond pulsed fiber laser system based on all-glass spun tapered double-clad fibers without employing any mitigating technique for the stimulated Brillouin scattering effect. The system delivers pulses with an 8 ns duration at a 100 kHz repetition rate, over 97.5% degree of polarization, a beam quality factor of M 2 ∼ 1 . 3 , a spectral linewidth of 53.8 MHz, a 160 W average power, and 188 kW peak power with a slope efficiency of 97.6%. The degree of spatial coherence of the amplified signal was measured to be 0.94. Our results are highly valued in applications requiring high-energy, high-coherence pulses with spectral, spatial, and polarization characteristics in a compact system. • High energy/high peak power nanosecond pulsed fiber-based laser system with near-diffraction-limited beam quality. • High temporal and spatial coherence. • Efficient SBS suppression by a spun tapered double-clad fiber. • Compact, stable, all-fiber monolithic system ideal for field application.

Optical Fiber TechnologyVol. 96
Latvia University of Life Sciences and Technologies (LV), Tampere University of Applied Sciences (FI), Tampere University (FI), University of Eastern Finland (FI)
Openalex Percentile: Top 14%
Photonic Crystal and Fiber Optics
1.46
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