• Chinese Optics Letters
  • Vol. 14, Issue 11, 111402 (2016)
Chao Feng1、2, Zhaojun Liu2, Zhenhua Cong2, Xiaodong Xu3, Jun Xu4, Han Rao2, Fen Bai5, Ping Li2, 青圃 王1、2、*, and Jiaxiong Fang1、2
Author Affiliations
  • 1Advanced Research Center for Optics, Shandong University, Jinan 250100, China
  • 2School of Information Science & Engineering, Shandong University, Jinan 250100, China
  • 3Jiangsu Key Laboratory of Advanced Laser Material and Device, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
  • 4School of Physics Science and Engineering, Institute for Advance Study, Tongji University, Shanghai 200092, China
  • 5College of Science, China University of Petroleum (East China), Qingdao 266580, China
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    DOI: 10.3788/COL201614.111402 Cite this Article Set citation alerts
    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 Copy Citation Text show less
    Diagram of CW laser experimental setups.
    Fig. 1. Diagram of CW laser experimental setups.
    Z-type CWML laser experimental setups.
    Fig. 2. Z-type CWML laser experimental setups.
    W-type CWML laser experimental setups.
    Fig. 3. W-type CWML laser experimental setups.
    Function of CW laser output power and the absorbed pump power.
    Fig. 4. Function of CW laser output power and the absorbed pump power.
    Average output power of the Z-type mode-locked laser change with the 808 nm pump power.
    Fig. 5. Average output power of the Z-type mode-locked laser change with the 808 nm pump power.
    Z-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 200 μs, and 20 ms, respectively.
    Fig. 6. Z-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 200 μs, and 20 ms, respectively.
    AC trace of the Z-type mode-locked laser and the fitted result with a Gaussian function.
    Fig. 7. AC trace of the Z-type mode-locked laser and the fitted result with a Gaussian function.
    Spectrum of the Z-type cavity CWML laser.
    Fig. 8. Spectrum of the Z-type cavity CWML laser.
    Average output power of the W-type mode-locked laser change with the 808 nm pump power.
    Fig. 9. Average output power of the W-type mode-locked laser change with the 808 nm pump power.
    W-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 20 μs, and 10 ms, respectively.
    Fig. 10. W-type cavity CWML laser pulse waveform at scanning times of 10 ns, 20 ns, 20 μs, and 10 ms, respectively.
    RF spectrum of the W-type cavity CWML laser.
    Fig. 11. RF spectrum of the W-type cavity CWML laser.
    Spectrum of the W-type cavity CWML laser.
    Fig. 12. Spectrum of the W-type cavity CWML laser.
    AC trace of the W-type CWML laser and the fitted result with a Gaussian function.
    Fig. 13. AC trace of the W-type CWML laser and the fitted result with a Gaussian function.
    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
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