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Topological Insulator: <formula formulatype="inline"><tex Notation="TeX">$\hbox{Bi}_{2}\hbox{Te}_{3}$ </tex></formula> Saturable Absorber for the Passive Q-Switching Operation of an in-Band Pumped 1645-nm Er:YAG Ceramic Laser
155
Citations
26
References
2013
Year
Ceramic LaserEngineeringTopological MaterialsLaser ScienceLaser PhysicsLaser ApplicationsLaser MaterialLaser SimulationSuper-intense LasersTopological Quantum StateHigh-power LasersOptical AmplifierTopological PhysicsOptical PropertiesQuantum MaterialsPulse PowerOptical PumpingQuantum SciencePhotonicsPhysicsTopological MaterialLaser ClassificationPromising Saturable AbsorberTopological InsulatorCondensed Matter PhysicsApplied PhysicsOptoelectronicsSaturable Absorber
An in-band pumped 1.645-μm Er:YAG ceramic laser passively Q-switched by a topological insulator: Bi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> Te <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> saturable absorber is reported. The average output power could reach up to 210 mW, corresponding to a pulsewidth, a pulse repetition rate, and a per-pulse energy of 6.3 μs, 40.7 kHz, and 5.3 μJ, respectively. This result indicates that the topological insulator: Bi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> Te <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> could be a promising saturable absorber such as graphene, with potential applications for solid-state lasers.
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