Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub>/MoO<sub>3</sub> composite as saturable absorber for dissipative soliton 1.0 μm mode-locked fiber laser

Abstract This work demonstrated a passive mode-locked ytterbium-doped fiber laser operating at a 1-micron region. The saturable absorber incorporated was a Ti 3 C 2 T x /MoO 3 deposited on a D-shaped fiber, generating stable dissipative soliton in all normal dispersion regimes. The all-fiber ring cavity laser configuration generates mode-locked pulses with a repetition rate of 24.2 MHz, which was further verified on the radio frequency spectrum. The dissipative soliton spectrum was centered explicitly at 1031 nm with a spectral edge-to-edge bandwidth of ∼3.7 nm. The Ti 3 C 2 T x /MoO 3 saturable absorber provides mode-locked stability with ∼59 dB of signal-to-noise ratio. The Ti 3 C 2 T x /MoO 3 mode-locked laser was amplified up to 101 mW, corresponding to 4.1 nJ of single pulse energy.

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Publication Details

Journal
Physica Scripta
Published
2025-05-06
DOI
https://doi.org/10.1088/1402-4896/add4ac
Citations
3
Primary Topic
Advanced Fiber Laser Technologies
Type
article
Field-Weighted Citation Impact
3.74

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article

Ti3C2Tx/MoO3 composite as saturable absorber for dissipative soliton 1.0 μm mode-locked fiber laser

Muhamad Zharif Samion, Suresh Sagadevan, K. Thambiratnam, Bülend Ortaç et al.
3 citations
Physica Scripta
Advanced Fiber Laser Technologies
3.74
article

Ti3C2Tx/MoO3 composite as saturable absorber for dissipative soliton 1.0 μm mode-locked fiber laser

Muhamad Zharif Samion, Suresh Sagadevan, K. Thambiratnam, Bülend Ortaç, H. Ahmad, Muhammad Khairol Annuar Zaini, Maisarah Lutfi
article en
3 citations

Abstract

Abstract This work demonstrated a passive mode-locked ytterbium-doped fiber laser operating at a 1-micron region. The saturable absorber incorporated was a Ti 3 C 2 T x /MoO 3 deposited on a D-shaped fiber, generating stable dissipative soliton in all normal dispersion regimes. The all-fiber ring cavity laser configuration generates mode-locked pulses with a repetition rate of 24.2 MHz, which was further verified on the radio frequency spectrum. The dissipative soliton spectrum was centered explicitly at 1031 nm with a spectral edge-to-edge bandwidth of ∼3.7 nm. The Ti 3 C 2 T x /MoO 3 saturable absorber provides mode-locked stability with ∼59 dB of signal-to-noise ratio. The Ti 3 C 2 T x /MoO 3 mode-locked laser was amplified up to 101 mW, corresponding to 4.1 nJ of single pulse energy.

Physica ScriptaVol. 100(6)
State University of Malang (ID), Bilkent University (TR), University of Malaya (MY), International Islamic University Malaysia (MY)
Ministry of Higher Education, Malaysia, Universiti Malaya
Openalex Percentile: Top 8%
Advanced Fiber Laser Technologies
3.74
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