Mode-locked laser based on doped fiber array
A mode-locked laser and doped fiber technology, applied in lasers, laser parts, phonon exciters, etc., can solve the problems of not being able to be all-fiber, unable to weld, difficult to couple gain fiber and fiber array, etc. Work efficiency, the effect of reducing post-process and loss
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Embodiment 1
[0040] Such as Figure 5 , the gain medium is an erbium-doped fiber array, and fiber gratings are used at both ends of the resonator as a cavity mirror. The pump light near 800nm, 980nm or 1480nm is absorbed when the pump light enters the erbium-doped fiber core on the way of internal reflection in the cladding, excites the ground state erbium ions, realizes the inversion of the upper energy level particles, and generates laser light in the resonant cavity . In the case of laser intensity fluctuations caused by slight vibrations, the weak light part will propagate to other cores, and the strong light part will continue to propagate in the doped fiber core due to nonlinear effects, reaching the Kerr mode-locking condition and obtaining a wavelength of 1.5 μm nearby ultrashort pulses.
Embodiment 2
[0042] Such as Figure 6 , the two ends of the ytterbium-doped fiber array are fused together, a coupler is added to it, and two couplers are fused, one coupler injects pump light with a wavelength near 915nm or 976nm, and the pump light is reflected in the cladding on the way When it enters the ytterbium-doped fiber core, it is absorbed, excites ytterbium ions in the ground state, realizes the inversion of the upper energy level particles, and generates laser light in the ring cavity. At the same time, the isolator can effectively prevent the reverse laser in the ring cavity. In the case of laser intensity fluctuations caused by slight vibrations, the weak light part will propagate into other cores, and the strong light part will continue to propagate in the doped fiber core due to nonlinear effects, reaching the Kerr mode-locking condition, with a wavelength of 1000nm- Ultrashort pulses around 1100nm are output from another coupler.
Embodiment 3
[0044] By changing the wavelength of the pump light in Example 1 to around 980-1051nm, the dopant element to praseodymium, and the fiber grating reflection center wavelength to around 1290-1315nm, the mode-locked pulse light output within this range can be obtained.
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