• Chinese Optics Letters
  • Vol. 16, Issue 11, 110501 (2018)
Zhiming Zhang, Wei Wei, Liqin Tang, Jie Yang, Jiewei Guo, Lei Ding, and Yigang Li*
Author Affiliations
  • School of Physics, Nankai University, Tianjin 300071, China
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    DOI: 10.3788/COL201816.110501 Cite this Article Set citation alerts
    Zhiming Zhang, Wei Wei, Liqin Tang, Jie Yang, Jiewei Guo, Lei Ding, Yigang Li. Generation of all-fiber femtosecond vortex laser based on NPR mode-locking and mechanical LPG[J]. Chinese Optics Letters, 2018, 16(11): 110501 Copy Citation Text show less
    Dispersion curves of LP01 and LP11; the relationship of the LPG period and the resonance wavelength.
    Fig. 1. Dispersion curves of LP01 and LP11; the relationship of the LPG period and the resonance wavelength.
    Converter producing and controlling the OAM modes.
    Fig. 2. Converter producing and controlling the OAM modes.
    Experimental setup. WDM: wavelength division multiplexing coupler; EDF: erbium-doped fiber; OC: optical coupler; PC: polarization controller; PD-ISO: polarization-dependent isolator; LPG: long period grating; CCD: charge coupled device, infrared camera; OSA: optical spectrum analyzer.
    Fig. 3. Experimental setup. WDM: wavelength division multiplexing coupler; EDF: erbium-doped fiber; OC: optical coupler; PC: polarization controller; PD-ISO: polarization-dependent isolator; LPG: long period grating; CCD: charge coupled device, infrared camera; OSA: optical spectrum analyzer.
    (a) Relationship between the pump power and output power of the laser in the continuous state (pentagon) or mode-locked state (circle). (b) The output spectrum of the laser running in the continuous state. (c) The output spectrum of the laser running in the mode-locked state. (d) The mode-locked pulse trains recorded by the oscilloscope. (e) The pulse recorded by autocorrelation and its fitting. (f) The infrared CCD image of the near-field intensity distribution: a1–f1 are when the laser is excited in the continuous state, a2–f2 are when the laser is running in the mode-locked state. a1 and a2 are LP01 modes, b1 and b2 are LP11 modes, c1, c2, e1, and e2 are in OAM modes with topological charges of +1 and −1, respectively; d1, d2, f1, and f2 are interference patterns of the corresponding OAM modes and reference beam.
    Fig. 4. (a) Relationship between the pump power and output power of the laser in the continuous state (pentagon) or mode-locked state (circle). (b) The output spectrum of the laser running in the continuous state. (c) The output spectrum of the laser running in the mode-locked state. (d) The mode-locked pulse trains recorded by the oscilloscope. (e) The pulse recorded by autocorrelation and its fitting. (f) The infrared CCD image of the near-field intensity distribution: a1–f1 are when the laser is excited in the continuous state, a2–f2 are when the laser is running in the mode-locked state. a1 and a2 are LP01 modes, b1 and b2 are LP11 modes, c1, c2, e1, and e2 are in OAM modes with topological charges of +1 and 1, respectively; d1, d2, f1, and f2 are interference patterns of the corresponding OAM modes and reference beam.
    Zhiming Zhang, Wei Wei, Liqin Tang, Jie Yang, Jiewei Guo, Lei Ding, Yigang Li. Generation of all-fiber femtosecond vortex laser based on NPR mode-locking and mechanical LPG[J]. Chinese Optics Letters, 2018, 16(11): 110501
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