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Based on the principle and fabrication of the optical waveguide laser,and through the configuration of the energy level of Er3+/Yb3+ co-doped system,the time-dependent rate equations are formed and then solved by Runge-Kutta algorithm.The dynamic characteristic of the waveguide laser pumped unidirec-tionally by 980 nm LD is analyzed.The curves of the relaxation oscillation are drawn,showing that the photon number and inverted population vary alternately.The attenuation characteristic of the peak power is studied.It is gained that time constant changes with pump power,length of waveguide and the reflectivity of output mirror.Furthermore,the impact of the above three parameters on the frequency and end-time of relaxation oscillation is discussed.The frequency of relaxation oscillation is propor-tional to the pump power.Under high reflectivity conditions,the length of waveguide has a weak impact on the frequency.The end-time decreases as the three parameters increase.These features and results provide a theoretical basis for designing the Er3+/Yb3+ co-doped phosphate optical waveguide laser.
Based on the principle and fabrication of the optical waveguide laser, and through the configuration of the energy level of Er3 + / Yb3 + co-doped system, the time-dependent rate equations are formed and then solved by Runge-Kutta algorithm. The dynamic characteristic of the waveguide laser pumped unidirecally by 980 nm LD is analyzed. The curves of the relaxation oscillation are drawn, showing that the photon number and inverted population vary alternately. attenuation characteristic of the peak power is studied. It is gain that time constant changes with pump power, length of waveguide and the reflectivity of output mirror. Focus of the impact of the above three parameters on the frequency and end-time of relaxation oscillation is discussed. frequency of relaxation oscillation is propor-tional to the pump power .Under high reflectivity conditions, the length of waveguide has a weak impact on the frequency.The end-time decreases as the three parameters increase.These features and re sults provide a theoretical basis for designing the Er3 + / Yb3 + co-doped phosphate optical waveguide laser.