Chinese Journal of Lasers, Volume. 47, Issue 6, 601002(2020)
Tunable Nd 3+∶YAG/KTiOAsO4 Raman Lasers
Fig. 6. Wavelengths of SPS Stokes laser and its first-order Raman laser versus phase-matching angle θ
Fig. 9. Powers of SPS Stokes laser and first-order Raman laser versus incident pumping power with tuning angle of 5.60° and pulse repetition frequency of 5 kHz
Fig. 10. Powers of 1064.16 nm initial fundamental laser and residual fundamental laser versus incident pumping power
Fig. 11. Waveforms of pulses with different wavelengths. (a) 1064.16 nm initial fundamental laser; (b) 1064.16 nm residual fundamental laser, 1088.12 nm SPS Stokes laser, and 1116.34 nm Raman laser
Fig. 12. Spot patterns of lasers with different wavelengths. (a) 1064.16 nm initial fundamental laser; (b) 1064.16 nm residual fundamental laser; (c) 1088.12 nm SPS Stokes laser; (d) 1116.34 nm first-order Raman laser
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Xu Jinjin, Zhang Xingyu, Cong Zhenhua, Liu Zhaojun, Chen Xiaohan, Qin Zengguang, Gao Feilong, Wang Peng, Wang Zecheng, Ming Na. Tunable Nd 3+∶YAG/KTiOAsO4 Raman Lasers[J]. Chinese Journal of Lasers, 2020, 47(6): 601002
Category: laser devices and laser physics
Received: Dec. 10, 2019
Accepted: --
Published Online: Jun. 3, 2020
The Author Email: Xingyu Zhang (xyz@sdu.edu.cn)