• Chinese Optics Letters
  • Vol. 19, Issue 11, 111903 (2021)
Jiazhu Wang, Liang Jin*, Shangzhi Xie, Renyan Wang, He Zhang, Yingtian Xu, Xin Zhao, Yan Li, and Xiaohui Ma
Author Affiliations
  • National Key Laboratory on High-power Semiconductor Lasers, Changchun University of Science and Technology, Changchun 130022, China
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    DOI: 10.3788/COL202119.111903 Cite this Article Set citation alerts
    Jiazhu Wang, Liang Jin, Shangzhi Xie, Renyan Wang, He Zhang, Yingtian Xu, Xin Zhao, Yan Li, Xiaohui Ma. Vector dynamics of ultrafast cylindrical vector beams in a mode-locked fiber laser[J]. Chinese Optics Letters, 2021, 19(11): 111903 Copy Citation Text show less
    (a) Experimental configuration of all-fiber GVLVSs fiber laser; (b) oscilloscope traces of these GVLVSs along the two orthogonal polarization axes; (c) polarization-resolved spectrum of GVLVSs; (d) pulse duration of GVLVSs.
    Fig. 1. (a) Experimental configuration of all-fiber GVLVSs fiber laser; (b) oscilloscope traces of these GVLVSs along the two orthogonal polarization axes; (c) polarization-resolved spectrum of GVLVSs; (d) pulse duration of GVLVSs.
    (a)–(d) Oscilloscope trace and (e)–(h) RF spectrum of the output pulses at different pump power.
    Fig. 2. (a)–(d) Oscilloscope trace and (e)–(h) RF spectrum of the output pulses at different pump power.
    (a) Transmission spectrum of LP01 mode of the TM-LPFG; (b) the surface morphology of TM-LPFG (inset: enlarged part).
    Fig. 3. (a) Transmission spectrum of LP01 mode of the TM-LPFG; (b) the surface morphology of TM-LPFG (inset: enlarged part).
    Intensity profiles of ultrafast CVBs based on vector-locked and non-vector-locked solitons. (a) and (f) are radially and azimuthally polarization beams without a polarizer; (b)–(e) and (g)–(j) show the profiles of the output beam after passing through a linear polarizer. Arrow indicates the orientation of the linear polarizer.
    Fig. 4. Intensity profiles of ultrafast CVBs based on vector-locked and non-vector-locked solitons. (a) and (f) are radially and azimuthally polarization beams without a polarizer; (b)–(e) and (g)–(j) show the profiles of the output beam after passing through a linear polarizer. Arrow indicates the orientation of the linear polarizer.
    Output power of ultrafast CVBs depends on the incident power of vector and non-vector-locked solitons.
    Fig. 5. Output power of ultrafast CVBs depends on the incident power of vector and non-vector-locked solitons.
    Time evolution of solitons based on SMS, CNT, and NPR mode-locking in terms of (a), (c), (e) Stokes parameters at the Poincaré sphere and (b), (d), (f) intensities of orthogonally polarized modes.
    Fig. 6. Time evolution of solitons based on SMS, CNT, and NPR mode-locking in terms of (a), (c), (e) Stokes parameters at the Poincaré sphere and (b), (d), (f) intensities of orthogonally polarized modes.
    Polarization and intensity profiles of ultrafast CVBs: (a) radial polarization TM01, (b) angular polarization TE01.
    Fig. 7. Polarization and intensity profiles of ultrafast CVBs: (a) radial polarization TM01, (b) angular polarization TE01.
    Jiazhu Wang, Liang Jin, Shangzhi Xie, Renyan Wang, He Zhang, Yingtian Xu, Xin Zhao, Yan Li, Xiaohui Ma. Vector dynamics of ultrafast cylindrical vector beams in a mode-locked fiber laser[J]. Chinese Optics Letters, 2021, 19(11): 111903
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