• Chinese Optics Letters
  • Vol. 16, Issue 2, 020015 (2018)
Yongjing Wu1, Siyuan Pang3、4, Yuqian Zu1, Qianqian Peng1, Jimin Yang1, Jie Liu1、2、*, and Liangbi Su3、4
Author Affiliations
  • 1Shandong Provincial Key Laboratory of Optics and Photonic Device, School of Physics and Electronics, Shandong Normal University, Jinan 250014, China
  • 2Institute of Data Science and Technology, Shandong Normal University, Jinan 250014, China
  • 3Synthetic Single Crystal Research Center, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201800, China
  • 4Key Laboratory of Transparent and Opto-functional Inorganic Materials, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201800, China
  • show less
    DOI: 10.3788/COL201816.020015 Cite this Article Set citation alerts
    Yongjing Wu, Siyuan Pang, Yuqian Zu, Qianqian Peng, Jimin Yang, Jie Liu, Liangbi Su. Silver nanorods absorber for passively Q-switched Nd,Gd:CaF2 laser[J]. Chinese Optics Letters, 2018, 16(2): 020015 Copy Citation Text show less
    (a) TEM image of the SNRs SA with a scale bar of 500 nm; (b) the absorption intensity coefficient of the SNRs SA; (c) a photograph of SNRs solution; (d) the nonlinear transmission curve of the SNRs SA.
    Fig. 1. (a) TEM image of the SNRs SA with a scale bar of 500 nm; (b) the absorption intensity coefficient of the SNRs SA; (c) a photograph of SNRs solution; (d) the nonlinear transmission curve of the SNRs SA.
    Schematics of diode-pumped Nd,Gd:CaF2 lasers in the CW mode and the PQS mode.
    Fig. 2. Schematics of diode-pumped Nd,Gd:CaF2 lasers in the CW mode and the PQS mode.
    (Color online) Average output power versus the absorbed pump power for CW.
    Fig. 3. (Color online) Average output power versus the absorbed pump power for CW.
    (Color online) Average output power, pulse width, repetition rate, and single pulse energy of the Q-switched Nd, Gd:CaF2 laser versus the absorbed pump power.
    Fig. 4. (Color online) Average output power, pulse width, repetition rate, and single pulse energy of the Q-switched Nd, Gd:CaF2 laser versus the absorbed pump power.
    Laser emission spectrum of the Q-switched pulse trains with T=3%; (a) the instability of the average output power measured during the 40 min with T=3%; (b) the beam quality of the Q-switched laser with T=3%; (c) the spatial beam profile of the Q-switched laser with T=3%.
    Fig. 5. Laser emission spectrum of the Q-switched pulse trains with T=3%; (a) the instability of the average output power measured during the 40 min with T=3%; (b) the beam quality of the Q-switched laser with T=3%; (c) the spatial beam profile of the Q-switched laser with T=3%.
    Typical pulse trains of the Q-switched laser in different time scales
    Fig. 6. Typical pulse trains of the Q-switched laser in different time scales
    Transmission of the OCT=2%T=3%
    Maximum average output power118 mW116 mW
    slope efficiency12.5%12.6%
    Repetition rate51.48 kHz53.92 kHz
    Shortest pulse width1.239 μs1.046 μs
    Single pulse energy2.29 μJ2.15 μJ
    Peak power1.85 W2.06 W
    Table 1. Results of the Q-switched Nd, Gd:CaF2 Laser Obtained with T= 2% and 3%
    Yongjing Wu, Siyuan Pang, Yuqian Zu, Qianqian Peng, Jimin Yang, Jie Liu, Liangbi Su. Silver nanorods absorber for passively Q-switched Nd,Gd:CaF2 laser[J]. Chinese Optics Letters, 2018, 16(2): 020015
    Download Citation