An end pumped Nd:YAP laser at 1341 nm is actively mode locked and passively Q-switched. Pumping was done with a pulsed high power laser diode with maximum power 425 W. V 3+ :YAG with 61% initial transmission served as saturable absorber, and an acousto-optic modulator is used for active mode locking
CW and passively Q-switching characteristics of a diode-end-pumped Nd:GGG laser at 1331 nm
โ Scribed by C.H. Zuo; B.T. Zhang; J.L. He; X.L. Dong; K.J. Yang; H.T. Huang; J.L. Xu; S. Zhao; C.M. Dong; X.T. Tao
- Publisher
- Elsevier Science
- Year
- 2009
- Tongue
- English
- Weight
- 281 KB
- Volume
- 31
- Category
- Article
- ISSN
- 0925-3467
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โฆ Synopsis
In this paper, continuous wave (CW) and passive Q-switching characteristics of a diode-end-pumped Nd:GGG laser at 1331 nm have been demonstrated. The maximum CW output power of 2.08 W was obtained under the incident pump power of 11 W, and the maximum slope efficiency and optical-optical conversion efficiency were 20.5% and 19%, respectively. By using a V 3+ :YAG crystal with initial transmission of 94% as the saturable absorber, the maximum average output power of the passively Q-switched laser at 1331 nm was 460 mW, and the minimum pulse width of 19 ns and the repetition rate of 39 kHz were achieved, corresponding to pulse peak power of 0.62 kW and single pulse energy of 11.8 lJ, respectively.
๐ SIMILAR VOLUMES
Pulsed UV lasers at the wavelengths of 374 and 280 nm are realized by cascaded second harmonic generation (SHG) and sum frequency generation (SFG) processes using a Nd:YAG laser at 1123 nm. The Nd:YAG laser is longitudinally pumped and passively Q-switched, and it has a high peak power of 3.2 kW. Th