Mode-Locking and Q-Switching in Holmium Doped Fiber Laser Using Topological Insulator (Sb₂Te₃) as Saturable Absorber

This work demonstrates mode-locking and Q-switching in a holmium-doped fiber laser (HDFL) using topological insulator (TI) antimony telluride (Sb2Te3) as the saturable absorber (SA). The TI was drop-casted on an arc-shaped fiber to generate mode-locked pulses and used in thin-film form to generate Q-switched pulses. The mode-locked pulses obtained were centered at 2081.1 nm with a repetition rate of 13.4 MHz, signal-to-noise ratio of 42 dB, and 1.85 ps pulse width. The Q-switched pulses were generated at the center wavelength of 2086.3 nm within the pump power of 1.55 W until 1.80 W. Within this range, the repetition rate peaked at 50.76 kHz and the pulse width dropped to a minimum value of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$2.64~\mu $ </tex-math></inline-formula>s. To the best of the author’s knowledge, this is the first work to use a topological insulator in an HDFL to generate both mode-locked and Q-switched pulses.

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Publication Details

Journal
IEEE Journal of Quantum Electronics
Published
2024-09-09
DOI
https://doi.org/10.1109/jqe.2024.3456073
Citations
6
Primary Topic
Advanced Fiber Laser Technologies
Type
article
Field-Weighted Citation Impact
2.03

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article

Mode-Locking and Q-Switching in Holmium Doped Fiber Laser Using Topological Insulator (Sb₂Te₃) as Saturable Absorber

Muhamad Zharif Samion, H. Ahmad, Khalil Kamaruzzaman
6 citations
IEEE Journal of Quantum Electronics
Advanced Fiber Laser Technologies
2.03
article

Mode-Locking and Q-Switching in Holmium Doped Fiber Laser Using Topological Insulator (Sb₂Te₃) as Saturable Absorber

Muhamad Zharif Samion, H. Ahmad, Khalil Kamaruzzaman
article en
6 citations

Abstract

This work demonstrates mode-locking and Q-switching in a holmium-doped fiber laser (HDFL) using topological insulator (TI) antimony telluride (Sb2Te3) as the saturable absorber (SA). The TI was drop-casted on an arc-shaped fiber to generate mode-locked pulses and used in thin-film form to generate Q-switched pulses. The mode-locked pulses obtained were centered at 2081.1 nm with a repetition rate of 13.4 MHz, signal-to-noise ratio of 42 dB, and 1.85 ps pulse width. The Q-switched pulses were generated at the center wavelength of 2086.3 nm within the pump power of 1.55 W until 1.80 W. Within this range, the repetition rate peaked at 50.76 kHz and the pulse width dropped to a minimum value of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$2.64~\mu $ </tex-math></inline-formula>s. To the best of the author’s knowledge, this is the first work to use a topological insulator in an HDFL to generate both mode-locked and Q-switched pulses.

IEEE Journal of Quantum ElectronicsVol. 60(6)
University of Malaya (MY)
Ministry of Higher Education, Malaysia, Universiti Malaya
Affordable and clean energy
Openalex Percentile: Top 13%
Advanced Fiber Laser Technologies
2.03
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Mode-Locking and Q-Switching in Holmium Doped Fiber Laser Using Topological Insulator (Sb₂Te₃) as Saturable Absorber — Muhamad Zharif Samion, H. Ahmad, et al. · IEEE Journal of Quantum Electronics (2024) | TGRS Research Map | TGRS