• Chinese Optics Letters
  • Vol. 18, Issue 1, 011401 (2020)
Yafei Wang1, Xingyu Li1, Jiamin Wu1, Xiulin Peng1, Jiangkun Cao1, Changsheng Yang1, Shanhui Xu1、2, Zhongmin Yang1, and Mingying Peng1、2、*
Author Affiliations
  • 1State Key Laboratory of Luminescent Materials and Devices, Guangdong Provincial Key Laboratory of Fiber Laser Materials and Applied Techniques, Guangdong Engineering Technology Research and Development Center of Special Optical Fiber Materials and Devices, School of Materials Science and Technology, South China University of Technology, Guangzhou 510640, China
  • 2Guangdong Engineering Technology Research and Development Center of High-performance Fiber Laser Techniques and Equipments, Zhuhai 519031, China
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    DOI: 10.3788/COL202018.011401 Cite this Article Set citation alerts
    Yafei Wang, Xingyu Li, Jiamin Wu, Xiulin Peng, Jiangkun Cao, Changsheng Yang, Shanhui Xu, Zhongmin Yang, Mingying Peng. Three-level all-fiber laser at 915 nm based on polarization-maintaining Nd3+-doped silica fiber[J]. Chinese Optics Letters, 2020, 18(1): 011401 Copy Citation Text show less
    (a) Setup of the gain coefficient measurement at 915 nm of the Nd3+-doped silica fiber. (b) Net gains versus pump powers of a 4.5 cm Nd3+-doped silica fiber for different signal powers (Ps).
    Fig. 1. (a) Setup of the gain coefficient measurement at 915 nm of the Nd3+-doped silica fiber. (b) Net gains versus pump powers of a 4.5 cm Nd3+-doped silica fiber for different signal powers (Ps).
    (a) The experimental setup of 915 nm Nd3+-doped silica fiber laser. (b) 915 nm laser spectrum of Nd3+-doped silica fiber. The inset is the energy level of Nd3+. (c) The laser output power with different lengths of gain fiber versus pump power (CE: optical-to-optical conversion efficiency).
    Fig. 2. (a) The experimental setup of 915 nm Nd3+-doped silica fiber laser. (b) 915 nm laser spectrum of Nd3+-doped silica fiber. The inset is the energy level of Nd3+. (c) The laser output power with different lengths of gain fiber versus pump power (CE: optical-to-optical conversion efficiency).
    Dependence of optical-to-optical conversion efficiency on the reflectivity of LR-FBG (70%, 83%, 90%) with a 5.1 cm fiber length.
    Fig. 3. Dependence of optical-to-optical conversion efficiency on the reflectivity of LR-FBG (70%, 83%, 90%) with a 5.1 cm fiber length.
    (a) Laser spectrum with a 0.02 nm OSA resolution. The inset is the output laser power versus the launched pump power. (b) The longitudinal-mode properties of DBR 915 nm fiber laser measured by FPI. (c) A brief schematic diagram of reducing the number of longitudinal modes in the DBR cavity.
    Fig. 4. (a) Laser spectrum with a 0.02 nm OSA resolution. The inset is the output laser power versus the launched pump power. (b) The longitudinal-mode properties of DBR 915 nm fiber laser measured by FPI. (c) A brief schematic diagram of reducing the number of longitudinal modes in the DBR cavity.
    Yafei Wang, Xingyu Li, Jiamin Wu, Xiulin Peng, Jiangkun Cao, Changsheng Yang, Shanhui Xu, Zhongmin Yang, Mingying Peng. Three-level all-fiber laser at 915 nm based on polarization-maintaining Nd3+-doped silica fiber[J]. Chinese Optics Letters, 2020, 18(1): 011401
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