A dual-wavelength, two-stage Yb-doped fiber amplification system is theoretically studied for further mid-infrared generation. In this amplification system, two sections of double-clad single-mode Yb-doped fiber are used as the gain medium, and the spectrum in the wavelength range 1000-1120 nm is simulated. For the simulation of the preamplification stage, a 975 nm diode laser with a power of 6.5 W is used to pump the preamplification stage by the counter-pumping scheme, and the measured dual-wavelength seed spectra are used. For the main amplification stage simulation, the gain fiber length is 1.7 m, and a 975 nm, 7.5 W diode laser is used as the pump source. Results show that for the two-stage amplification process, the maximum value of the dual-wavelength power product can be obtained in the main amplification stage with a 1.7 m gain fiber when the 2.2 m Yb-doped fiber is selected for the preamplification stage with the counter-pumping scheme. Under the above condition, the total average power of the seed signal after amplification is calculated to be 3.2 W, with negligible ASE noise. In addition, we have compared the theoretically calculated spectral results with the experimental results of the actual main amplification stage.
In this paper, the rate equation of ytterbium ion concentration in the upper level and the transmission equations of seed signal, pump, and amplified spontaneous emission (ASE) are solved simultaneously by the explicit Runge Kutta method. Finally, a full spectral range of 1000~1130 nm seed power spectrum simulation is achieved. This paper focuses on the amplification of the seed signal at different peak wavelengths in different fiber lengths. The main works are as follows:The accuracy of calculation results by the iterative method has been improved. By constructing 3D data structure of seed signal, a parallel computing work on the propagation process of Gaussian-lineshape seed spectrum with a peak wavelength of 1020-1100 nm in ytterbium-doped fiber with a length of 1-30 m has been done, which makes the calculation time is significantly reduced. Finally, the reabsorption effect of seed signal at different peak wavelengths and the competition between the seed signal and ASE has been analyzed, and the optimal gain fiber length corresponding to the different peak wavelengths of the seed signal has also been discussed.
An all-fiber wavelength-tunable narrow-linewidth polarization-maintaining (PM) Tm-doped fiber master oscillator power amplifier (MOPA) system is presented. We demonstrate an all-fiber ring cavity Tm-doped fiber master-oscillator (MO) with a tuning range of 110 nm (from 1925 to 2034 nm). The maximum output power of 459 mW is obtained at 1992.9 nm for 16 W of launched pump power at 793 nm, corresponding to a slope efficiency of 5.6% concerning launched pump power. By using a one-stage Tm-doped fiber amplifier combined with a high gain of >10 dB, the maximum slope efficiency is 12.6% and the output power is 5.65 W at 1993 nm. The 3 dB linewidth is less than 0.5 nm, M2 ≈ 1.25, and the polarization extinction ratio (PER) reaches 21.4 dB. The influence of different active fiber lengths on laser amplification is also studied.
We systematically studied several of the most traditional hollow-core anti-resonant fiber (HC-ARF) structures, with the aim of achieving low confinement loss, single-mode performance, and high insensitivity to bending in the 2 µm band. Moreover, the propagation loss of fundamental mode (FM), higher-order mode (HOMs), and the higher-order mode extinction ratio (HOMER) under different geometric parameters were studied. Analysis showed that the confinement loss of the six-tube nodeless hollow-core anti-resonant fiber at 2 µm was 0.042 dB/km, and its higher-order mode extinction ratio was higher than 9000. At the same time, a confinement loss of 0.040 dB/km at 2 was is achieved in the five-tube nodeless hollow-core anti-resonant fiber, and its higher-order mode extinction ratio was higher than 2700.
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