Publication | Closed Access
1-, 1.5-, and 2-μm Fiber Lasers Q-Switched by a Broadband Few-Layer MoS<sub>2</sub> Saturable Absorber
340
Citations
60
References
2014
Year
Materials SciencePhotonicsPolyvinyl AlcoholEngineeringLaser ScienceOptoelectronic MaterialsApplied PhysicsLaser ApplicationsPhotonic MaterialsLaser ClassificationLaser MaterialSuper-intense LasersLaser MaterialsNonlinear Saturable AbsorptionOptoelectronicsHigh-power LasersFiber LaserFew-layer Molybdenum Sulfide
We propose and demonstrate 1, 1.5, and 2 μm passively Q-switched fiber lasers by exploiting a few-layer Molybdenum sulfide (MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> ) polymer composite as broadband saturable absorber (SA), respectively. The few-layer MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> nanosheets are prepared by the liquid-phase exfoliation method, and are composited with polyvinyl alcohol (PVA). The PVA-MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> film is sandwiched between two fiber ferrules to form the fiber-compatible SA. The few-layer MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> not only shows good transparency from ultraviolet to mid-infrared spectral region, but also possesses the nonlinear saturable absorption. The modulation depth and saturation optical intensity of the PVA-MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> film are measured to be 1.6% and 13 MW/cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> at 1566 nm by the balanced twin-detector technique, respectively. By further inserting the filmy PVA-MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> SA into the cavities of Yb-, Er- and Tm-doped fiber lasers, we achieve stable Q-switching operations at 1.06, 1.56, and 2.03 μm, respectively. The output characteristics of the Q-switched pulses at the three wavelengths have been investigated, respectively. The MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -based Q-switching enables the large pulse energy of ~1 μJ with a pulse width of 1.76 μs. This is, to the best of our knowledge, the first demonstration of MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -based Q-switched fiber lasers in a wide wavelength range (from 1 to 2 μm). Our results experimentally confirm that the new-type 2-D material, few-layer MoS <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> , is a promising broadband SA to Q-switch fiber lasers covering all major wavelengths from near- to mid-infrared region.
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