Author Affiliations
1Shanghai Jiao Tong University, School of Physics and Astronomy, Shanghai, China2Shanghai Jiao Tong University, Collaborative Innovation Center of Inertial Fusion Sciences and Applications, Shanghai, China3Shanghai Jiao Tong University, Key Laboratory for Laser Plasmas, Ministry of Education, Shanghai, Chinashow less
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.
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; , half-wave plate; , quarter-wave plate; and Ge, germanium rod.
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.
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 , , , and 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. 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.