• Chinese Optics Letters
  • Vol. 21, Issue 2, 021405 (2023)
Jingjing Zhou1, Changsheng Zheng1, Bin Chen2、3, Ning Zhang2、3, Qinggang Gao2、3, Hangqi Yuan1, Daiwen Jia1, Zhanxin Wang1、*, Shande Liu2, Yuping Zhang2, Huiyun Zhang2, and Yongguang Zhao1、3、**
Author Affiliations
  • 1Jiangsu Key Laboratory of Advanced Laser Materials and Devices, Jiangsu Normal University, Xuzhou 221116, China
  • 2College of Electronic and Information Engineering, Shandong University of Science and Technology, Qingdao 266590, China
  • 3Jiangsu Collaborative Innovation Center of Advanced Laser Technology and Emerging Industry, Jiangsu Normal University, Xuzhou 221116, China
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    DOI: 10.3788/COL202321.021405 Cite this Article Set citation alerts
    Jingjing Zhou, Changsheng Zheng, Bin Chen, Ning Zhang, Qinggang Gao, Hangqi Yuan, Daiwen Jia, Zhanxin Wang, Shande Liu, Yuping Zhang, Huiyun Zhang, Yongguang Zhao. Widely tunable 2 µm optical vortex from a Tm:YAP laser[J]. Chinese Optics Letters, 2023, 21(2): 021405 Copy Citation Text show less
    (a) Calculated effective pumping areas versus cavity length for different LG modes with an annular pump. (b) Schematic of the 2 µm wavelength-tunable Tm:YAP vortex laser. LD, laser diode; L, lens; IM, input mirror; BF, birefringent filter; OC, output coupler.
    Fig. 1. (a) Calculated effective pumping areas versus cavity length for different LG modes with an annular pump. (b) Schematic of the 2 µm wavelength-tunable Tm:YAP vortex laser. LD, laser diode; L, lens; IM, input mirror; BF, birefringent filter; OC, output coupler.
    (a) Laser slope efficiency, (b) wavelength tuning performance, and (c) the polarization measurement of the annular light pumped Tm:YAP laser with E∥b and E∥c polarization. Inset in (a): beam pattern and the corresponding optical spectrum of the Tm:YAP laser without BF.
    Fig. 2. (a) Laser slope efficiency, (b) wavelength tuning performance, and (c) the polarization measurement of the annular light pumped Tm:YAP laser with E∥b and E∥c polarization. Inset in (a): beam pattern and the corresponding optical spectrum of the Tm:YAP laser without BF.
    Simulated beam radius of laser in the YAP crystal as a function of absorbed pump power by considering the thermal lens effect. Inset: beam profiles of the output laser at different pump powers.
    Fig. 3. Simulated beam radius of laser in the YAP crystal as a function of absorbed pump power by considering the thermal lens effect. Inset: beam profiles of the output laser at different pump powers.
    (a) Laser output performance of the LG0,+1 modes with and without the BF. (b) Beam profiles and the corresponding interference fringe patterns of LG0,+1 and LG0,-1 modes. Insets in (a): optical spectra and polarization measurement of LG0,+1 and LG0,-1 modes without the BF in the cavity.
    Fig. 4. (a) Laser output performance of the LG0,+1 modes with and without the BF. (b) Beam profiles and the corresponding interference fringe patterns of LG0,+1 and LG0,-1 modes. Insets in (a): optical spectra and polarization measurement of LG0,+1 and LG0,-1 modes without the BF in the cavity.
    (a) Measured tuning spectra for LG0,+1 and LG0,-1 modes at the fixed absorbed pump power of 4.27 W. (b) and (c) The measured spectral lines at several typical wavelengths for the LG0,+1 and LG0,-1 modes.
    Fig. 5. (a) Measured tuning spectra for LG0,+1 and LG0,-1 modes at the fixed absorbed pump power of 4.27 W. (b) and (c) The measured spectral lines at several typical wavelengths for the LG0,+1 and LG0,-1 modes.
    Jingjing Zhou, Changsheng Zheng, Bin Chen, Ning Zhang, Qinggang Gao, Hangqi Yuan, Daiwen Jia, Zhanxin Wang, Shande Liu, Yuping Zhang, Huiyun Zhang, Yongguang Zhao. Widely tunable 2 µm optical vortex from a Tm:YAP laser[J]. Chinese Optics Letters, 2023, 21(2): 021405
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