“…11) SA cladding is also widely used to prevent transverse lasing in disk or slab amplifiers. [12][13][14][15] In this letter, we consider that an SA-inserted between the gain medium and the return mirror of a nanosecond doublepass amplifier can effectively absorb the ASE until the seed pulse arrive. To evaluate the effectiveness of this method, we develop a theoretical model for the SA-inserted double-pass amplifier by combining existing the SA model 16) with the modified Frantz-Nodvik equation.…”
We propose the insertion of a saturable absorber (SA) in a nanosecond double-pass laser amplifier as an amplified spontaneous emission (ASE) suppressor. To analyze the influence of the SA, a theoretical model is developed. One-dimensional simulation results show reasonable agreement with measurements in terms of the output energy and temporal pulse shape. For our amplifier parameters, when an SA of initial transmission 0.5 is inserted, the simulation anticipates the ASE to be reduced by a factor of 0.37 while the output pulse energy is maintained.
“…11) SA cladding is also widely used to prevent transverse lasing in disk or slab amplifiers. [12][13][14][15] In this letter, we consider that an SA-inserted between the gain medium and the return mirror of a nanosecond doublepass amplifier can effectively absorb the ASE until the seed pulse arrive. To evaluate the effectiveness of this method, we develop a theoretical model for the SA-inserted double-pass amplifier by combining existing the SA model 16) with the modified Frantz-Nodvik equation.…”
We propose the insertion of a saturable absorber (SA) in a nanosecond double-pass laser amplifier as an amplified spontaneous emission (ASE) suppressor. To analyze the influence of the SA, a theoretical model is developed. One-dimensional simulation results show reasonable agreement with measurements in terms of the output energy and temporal pulse shape. For our amplifier parameters, when an SA of initial transmission 0.5 is inserted, the simulation anticipates the ASE to be reduced by a factor of 0.37 while the output pulse energy is maintained.
We demonstrate a master oscillator power amplifier (MOPA) architecture based on Yb:YAG amplifiers and adaptive optics (AO) systems with a high power and high beam quality laser output. With two conduction cooled, dual-end-pumped Yb:YAG zigzag-slab amplifiers at room temperature, the fiber laser of 300 W was scaled to 11.9 kW. Moreover, AO system positioned downstream was utilized to correct wavefront of amplified laser. The beam quality at maximum output power was 2.8 times diffraction limited with closed-loop AO system.
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