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1.7  µm Tm-fiber chirped pulse amplification system with dissipative soliton seed laser

Jixiang Chen, Ze-Yu Zhan, Can Li, Meng Liu, Ai‐Ping Luo, Pu Zhou, Wen‐Cheng Xu, Zhi‐Chao Luo

2021Optics Letters28 citationsDOI

Abstract

We report on a 1.7 µm Tm-fiber chirped pulse amplification (CPA) system by virtue of a broadband dissipative soliton seed laser. The seed oscillator delivers the dissipative soliton with 10 dB spectral bandwidth of 23 nm and an average power of 4 mW. The duration of the seed pulse is directly stretched to <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:mo>∼</mml:mo> </mml:mrow> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:mn>60</mml:mn> </mml:mrow> <mml:mspace width="thickmathspace"/> <mml:mrow class="MJX-TeXAtom-ORD"> <mml:mi mathvariant="normal">p</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> </mml:mrow> </mml:math> by a segment of 50 m normal dispersion fiber. Using a two-stage fiber amplifier, the average power of the pulse is amplified to 1.95 W with a slope efficiency of 40.3%. The amplified pulse is then compressed to 348 fs by a pair of fused silica transmission gratings. The compressed average power of 1.3 W and peak power of 155 kW are achieved. These experimental results would pave the way to achieve a high-power femtosecond laser source at 1.7 µm, which could find important applications in fields such as three-photon deep-tissue imaging and material processing.

Topics & Concepts

OpticsChirped pulse amplificationFiber laserDissipative solitonLaserUltrashort pulseMaterials sciencePulse (music)Pulse shapingFemtosecond pulse shapingOptical fiberSelf-phase modulationSolitonPhysicsNonlinear opticsNonlinear systemDetectorQuantum mechanicsAdvanced Fiber Laser TechnologiesLaser-Matter Interactions and ApplicationsPhotonic Crystal and Fiber Optics
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