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340 mW nanosecond compact 1.7 μm passively Q-switched laser based on a fiber-type saturable absorber with mismatch of mode-field area
Centre for Optical and Electromagnetic Research, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310058, China; Zhejiang Engineering Research Center for Intelligent Medical Imaging, Sensing and Non-invasive Rapid Testing, Taizhou Hospital, Zhejiang University, Taizhou 318000, China.
KTH, School of Electrical Engineering and Computer Science (EECS), Electrical Engineering, Electromagnetic Engineering and Fusion Science. Zhejiang Engineering Research Center for Intelligent Medical Imaging, Sensing and Non-invasive Rapid Testing, Taizhou Hospital, Zhejiang University, Taizhou 318000, China; National Engineering Research Center for Optical Instruments, Zhejiang University, Hangzhou 310058, China; Department of Electromagnetic Engineering, School of Electrical Engineering.ORCID iD: 0000-0002-3401-1125
2025 (English)In: Optics and Laser Technology, ISSN 0030-3992, E-ISSN 1879-2545, Vol. 184, article id 112511Article in journal (Refereed) Published
Abstract [en]

Here, we report a passively Q-switched Tm laser at 1720 nm. The Q-switching behavior originates from a piece of Tm-doped fiber. Tm-doped fiber has a broad absorption spectrum covering 1.7 μm waveband, which can be used as a fiber-type saturable absorber for 1.7 μm pulsed lasers. In comparison with the typical Q-switching system in which the gain fiber has a different rare-earth doping from the fiber-type saturable absorber, the same rare-earth doping in the gain fiber and the saturable absorber cannot support the effective Q-switching operation. To initiate the pulsing operation in this Tm-Tm laser system, we introduce a mismatch of mode-field area between the gain fiber and the fiber-type saturable absorber. By using ∼50 cm Tm-doped fibers as the saturable absorber, the passive Q-switching 1720 nm laser is realized and produces 340 mW output power with a nanosecond pulse width (400 ns ∼422 ns). After investigating the Q-switching pulses, it is found that the evolution trend of the pulses with the pump power is not consistent with the typical passive Q-switching lasers. In order to understand this unusual Q-switching behavior, we establish a rate equation model that is coupled with the mismatch of mode-field area to give a comprehensive understanding. From the numerical simulation, a new Q-switching laser cavity consisting of dual laser resonance is proposed to guide how to realize a passive Q-switching 1.7 μm laser with a higher output power.

Place, publisher, year, edition, pages
Elsevier BV , 2025. Vol. 184, article id 112511
National Category
Physical Sciences
Identifiers
URN: urn:nbn:se:kth:diva-359670DOI: 10.1016/j.optlastec.2025.112511ISI: 001413241400001Scopus ID: 2-s2.0-85216125088OAI: oai:DiVA.org:kth-359670DiVA, id: diva2:1935414
Note

QC 20250226

Available from: 2025-02-06 Created: 2025-02-06 Last updated: 2025-02-26Bibliographically approved

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