1. Passive Q-switching of microchip lasers based on Ho:YAG ceramics
- Author
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Li Junlin, Uwe Griebner, Konstantin Yumashev, Fabian Rotermund, A.S. Yasukevich, Pavel Loiko, Mi Hye Kim, Xavier Mateos, Sun Young Choi, Valentin Petrov, Yicheng Wang, Ruijun Lan, and Yubai Pan
- Subjects
Materials science ,business.industry ,Graphene ,Materials Science (miscellaneous) ,Slope efficiency ,Pulse duration ,02 engineering and technology ,021001 nanoscience & nanotechnology ,Laser ,01 natural sciences ,Q-switching ,Industrial and Manufacturing Engineering ,law.invention ,010309 optics ,X-ray laser ,Optics ,law ,Fiber laser ,0103 physical sciences ,Continuous wave ,Optoelectronics ,Business and International Management ,0210 nano-technology ,business - Abstract
A Ho:YAG ceramic microchip laser pumped by a Tm fiber laser at 1910 nm is passively Q-switched by single- and multi-layer graphene, single-walled carbon nanotubes (SWCNTs), and Crsup2+/sup:ZnSe saturable absorbers (SAs). Employing SWCNTs, this laser generated an average power of 810 mW at 2090 nm with a slope efficiency of 68% and continuous wave to Q-switching conversion efficiency of 70%. The shortest pulse duration was 85 ns at a repetition rate of 165 kHz, and the pulse energy reached 4.9 μJ. The laser performance and pulse stability were superior compared to graphene SAs even for a different number of graphene layers (n=1 to 4). A model for the description of the Ho:YAG laser Q-switched by carbon nanostructures is presented. This modeling allowed us to estimate the saturation intensity for multi-layered graphene and SWCNT SAs to be 1.2±0.2 and 7±1 MW/cmsup2/sup, respectively. When using Crsup2+/sup:ZnSe, the Ho:YAG microchip laser generated 11 ns/25 μJ pulses at a repetition rate of 14.8 kHz.
- Published
- 2016