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Chinese Optics Letters, Volume. 14, Issue 11, 111402(2016)

Low threshold high stability passively mode-locked laser performance of a disordered crystal: Nd3+:Gd0.5Y2.5Al5O12

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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    Diagram of CW laser experimental setups.

    Fig. 1. Diagram of CW laser experimental setups.

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    Z-type CWML laser experimental setups.

    Fig. 2. Z-type CWML laser experimental setups.

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    W-type CWML laser experimental setups.

    Fig. 3. W-type CWML laser experimental setups.

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    Function of CW laser output power and the absorbed pump power.

    Fig. 4. Function of CW laser output power and the absorbed pump power.

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    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.

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    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.

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    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.

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    Spectrum of the Z-type cavity CWML laser.

    Fig. 8. Spectrum of the Z-type cavity CWML laser.

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    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.

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    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.

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    RF spectrum of the W-type cavity CWML laser.

    Fig. 11. RF spectrum of the W-type cavity CWML laser.

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    Spectrum of the W-type cavity CWML laser.

    Fig. 12. Spectrum of the W-type cavity CWML laser.

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    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.

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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," Chin. Opt. Lett. 14, 111402 (2016)

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    Paper Information

    Category: Lasers and Laser Optics

    Received: Jun. 28, 2016

    Accepted: Sep. 23, 2016

    Published Online: Aug. 2, 2018

    The Author Email: 青圃 王 (qpwang@sdu.edu.cn)

    DOI:10.3788/COL201614.111402

    Topics

    laser devices and laser physics
    Lasers and Laser Optics
    Laser physics
    laser manufacturing
    Instrumentation, Measurement and Metrology