Low threshold high stability passively mode-locked laser performance of a disordered crystal: Nd3+:Gd0.5Y2.5Al5O12
1 Advanced Research Center for Optics, Shandong University, Jinan 250100, China
2 School of Information Science & Engineering, Shandong University, Jinan 250100, China
3 Jiangsu Key Laboratory of Advanced Laser Material and Device, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
4 School of Physics Science and Engineering, Institute for Advance Study, Tongji University, Shanghai 200092, China
5 College of Science, China University of Petroleum (East China), Qingdao 266580, China
Figures & Tables
Fig. 1. Diagram of CW laser experimental setups.
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Fig. 2. Z-type CWML laser experimental setups.
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Fig. 3. W-type CWML laser experimental setups.
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Fig. 4. Function of CW laser output power and the absorbed pump power.
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Fig. 5. Average output power of the Z-type mode-locked laser change with the 808 nm pump power.
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Fig. 6. Z-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 200 μs, and 20 ms, respectively.
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Fig. 7. AC trace of the Z-type mode-locked laser and the fitted result with a Gaussian function.
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Fig. 8. Spectrum of the Z-type cavity CWML laser.
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Fig. 9. Average output power of the W-type mode-locked laser change with the 808 nm pump power.
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Fig. 10. W-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 20 μs, and 10 ms, respectively.
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Fig. 11. RF spectrum of the W-type cavity CWML laser.
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Fig. 12. Spectrum of the W-type cavity CWML laser.
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Fig. 13. AC trace of the W-type CWML laser and the fitted result with a Gaussian function.
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Chao Feng, Zhaojun Liu, Zhenhua Cong, Xiaodong Xu, Jun Xu, Han Rao, Fen Bai, Ping Li, 青圃 王, Jiaxiong Fang. Low threshold high stability passively mode-locked laser performance of a disordered crystal: Nd3+:Gd0.5Y2.5Al5O12[J]. Chinese Optics Letters, 2016, 14(11): 111402.