• Chinese Optics Letters
  • Vol. 13, Issue 2, 021404 (2015)
Yongguang Zhao1, Zhengping Wang2、*, Haohai Yu2, Xiaodong Xu3, Jun Xu3, and Xinguang Xu2
Author Affiliations
  • 1Key Laboratory of Advanced Laser Materials and Devices, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou 221116, China
  • 2State Key Laboratory of Crystal Materials and Institute of Crystal Materials, Shandong University, Jinan 250100, China
  • 3Key Laboratory of Transparent and Opto-Functional Inorganic Materials, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.3788/COL201513.021404 Cite this Article Set citation alerts
    Yongguang Zhao, Zhengping Wang, Haohai Yu, Xiaodong Xu, Jun Xu, Xinguang Xu. Efficient multi-wavelength lasers made of Nd:GdLuAG crystal[J]. Chinese Optics Letters, 2015, 13(2): 021404 Copy Citation Text show less
    Fluorescence spectrum of the Nd:GdLuAG crystal at room temperature. Inset: Fine spectrum of the F43/2→I413/2 transition.
    Fig. 1. Fluorescence spectrum of the Nd:GdLuAG crystal at room temperature. Inset: Fine spectrum of the F43/2I413/2 transition.
    Schematic diagram of the experimental setup, and the transmission of the different output couplers used in this experiment.
    Fig. 2. Schematic diagram of the experimental setup, and the transmission of the different output couplers used in this experiment.
    (a) Output power as a function of the absorbed pump power. (b) The calculated initial laser thresholds at different wavelengths, and the experimental results at 1338 nm.
    Fig. 3. (a) Output power as a function of the absorbed pump power. (b) The calculated initial laser thresholds at different wavelengths, and the experimental results at 1338 nm.
    Laser spectra at different absorbed pump powers when T=3.4%: (a) Pab=0.8 W. (b) Pab=3.2 W. (c) Pab=6.8 W. (d) Pab=9.42 W.
    Fig. 4. Laser spectra at different absorbed pump powers when T=3.4%: (a) Pab=0.8W. (b) Pab=3.2W. (c) Pab=6.8W. (d) Pab=9.42W.
    Characterization of the passive Q-switching laser. (a) Average output power versus the absorbed pump power. (b) Pulse width as a function of the absorbed pump power; inset: pulse profile of 21.8 ns. (c) Pulse energy versus the absorbed pump power. (d) Laser spectrum of the passive Q-switched dual-wavelength laser at the absorbed pump power of 9.42 W; inset: the pulse trains at 14.8 kHz.
    Fig. 5. Characterization of the passive Q-switching laser. (a) Average output power versus the absorbed pump power. (b) Pulse width as a function of the absorbed pump power; inset: pulse profile of 21.8 ns. (c) Pulse energy versus the absorbed pump power. (d) Laser spectrum of the passive Q-switched dual-wavelength laser at the absorbed pump power of 9.42 W; inset: the pulse trains at 14.8 kHz.
    Initial population inversion density versus the initial transmittance of the absorber and the output coupler (left). Total population inversion density at the different couplers (right).
    Fig. 6. Initial population inversion density versus the initial transmittance of the absorber and the output coupler (left). Total population inversion density at the different couplers (right).
    Yongguang Zhao, Zhengping Wang, Haohai Yu, Xiaodong Xu, Jun Xu, Xinguang Xu. Efficient multi-wavelength lasers made of Nd:GdLuAG crystal[J]. Chinese Optics Letters, 2015, 13(2): 021404
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