• Advanced Photonics
  • Vol. 1, Issue 6, 065001 (2019)
Zhipeng Qin1、2、3, Guoqiang Xie1、2、3、*, Hongan Gu1、2、3, Ting Hai1、2、3, Peng Yuan1、2、3, Jingui Ma1、2、3, and Liejia Qian1、2、3、*
Author Affiliations
  • 1Shanghai Jiao Tong University, School of Physics and Astronomy, Shanghai, China
  • 2Shanghai Jiao Tong University, Collaborative Innovation Center of Inertial Fusion Sciences and Applications, Shanghai, China
  • 3Shanghai Jiao Tong University, Key Laboratory for Laser Plasmas, Ministry of Education, Shanghai, China
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    DOI: 10.1117/1.AP.1.6.065001 Cite this Article Set citation alerts
    Zhipeng Qin, Guoqiang Xie, Hongan Gu, Ting Hai, Peng Yuan, Jingui Ma, Liejia Qian. Mode-locked 2.8-μm fluoride fiber laser: from soliton to breathing pulse[J]. Advanced Photonics, 2019, 1(6): 065001 Copy Citation Text show less
    (a) GVD and refractive-index curves of Ge and GVD curve of ZBLAN fiber. Sellmeier equations of Ge and ZBLAN are used from Refs. 18 and 19. (b) Transmission curve of 2-cm-long antireflection-coated Ge rod measured using a Fourier-transform spectrometer.
    Fig. 1. (a) GVD and refractive-index curves of Ge and GVD curve of ZBLAN fiber. Sellmeier equations of Ge and ZBLAN are used from Refs. 18 and 19. (b) Transmission curve of 2-cm-long antireflection-coated Ge rod measured using a Fourier-transform spectrometer.
    Schematic of the breathing-pulse mode-locked Er:ZBLAN fiber laser. LD, laser diode; DM, dichroic mirror; OC, output coupler with a transmission of 40%; ISO, optical isolator; λ/2, half-wave plate; λ/4, quarter-wave plate; and Ge, germanium rod.
    Fig. 2. Schematic of the breathing-pulse mode-locked Er:ZBLAN fiber laser. LD, laser diode; DM, dichroic mirror; OC, output coupler with a transmission of 40%; ISO, optical isolator; λ/2, half-wave plate; λ/4, quarter-wave plate; and Ge, germanium rod.
    Soliton mode-locked Er:ZBLAN fiber laser: (a) pulse trains in nanosecond and millisecond time scales, respectively; (b) radiofrequency spectrum; (c) measured intensity autocorrelation trace; and (d) mode-locked pulse spectrum.
    Fig. 3. Soliton mode-locked Er:ZBLAN fiber laser: (a) pulse trains in nanosecond and millisecond time scales, respectively; (b) radiofrequency spectrum; (c) measured intensity autocorrelation trace; and (d) mode-locked pulse spectrum.
    Characteristics of the breathing-pulse mode-locked Er:ZBLAN fiber laser. Evolution of (a) pulse energy and duration, (b) autocorrelation trace, and (c) mode-locking spectrum with the Ge rod length. The net intracavity dispersions are −0.191, −0.158, −0.141, and −0.090 ps2 for Ge rod lengths of 0, 2, 3, and 6 cm, respectively. Evolution of the (d) pulse energy and duration with the launched pump power in the soliton and breathing-pulse regimes. (e) Measured autocorrelation trace and (f) mode-locking spectrum for 9.3-nJ output pulses.
    Fig. 4. Characteristics of the breathing-pulse mode-locked Er:ZBLAN fiber laser. Evolution of (a) pulse energy and duration, (b) autocorrelation trace, and (c) mode-locking spectrum with the Ge rod length. The net intracavity dispersions are 0.191, 0.158, 0.141, and 0.090  ps2 for Ge rod lengths of 0, 2, 3, and 6 cm, respectively. Evolution of the (d) pulse energy and duration with the launched pump power in the soliton and breathing-pulse regimes. (e) Measured autocorrelation trace and (f) mode-locking spectrum for 9.3-nJ output pulses.
    Numerical simulation of a breathing-pulse MLFFL consisting of an NPR system, a Ge rod, an Er:ZBLAN fiber, and an OC. Evolution of (a) pulse duration, (b) spectrum, and (c) pulse energy along the cavity.
    Fig. 5. Numerical simulation of a breathing-pulse MLFFL consisting of an NPR system, a Ge rod, an Er:ZBLAN fiber, and an OC. Evolution of (a) pulse duration, (b) spectrum, and (c) pulse energy along the cavity.
    Zhipeng Qin, Guoqiang Xie, Hongan Gu, Ting Hai, Peng Yuan, Jingui Ma, Liejia Qian. Mode-locked 2.8-μm fluoride fiber laser: from soliton to breathing pulse[J]. Advanced Photonics, 2019, 1(6): 065001
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