wei xiao-feng, lu zhi-wei, huang xiao-jun, et al. Propagation of the super-Gaussian beam in Ti:sapphire CPA system[J]. High Power Laser and Particle Beams, 2005, 17.
Citation:
wei xiao-feng, lu zhi-wei, huang xiao-jun, et al. Propagation of the super-Gaussian beam in Ti:sapphire CPA system[J]. High Power Laser and Particle Beams, 2005, 17.
wei xiao-feng, lu zhi-wei, huang xiao-jun, et al. Propagation of the super-Gaussian beam in Ti:sapphire CPA system[J]. High Power Laser and Particle Beams, 2005, 17.
Citation:
wei xiao-feng, lu zhi-wei, huang xiao-jun, et al. Propagation of the super-Gaussian beam in Ti:sapphire CPA system[J]. High Power Laser and Particle Beams, 2005, 17.
In order to improve the filled factor of beam and the conversion efficiency of amplifier, with reference to the technical integrated line of Shenguang-Ⅲ, a kind of new spatial four-pass amplifier structure is designed, which is made up of four pairs of spatial filters, in the Ti:sapphire CPA system. The spatial structure amplifier is put in a vacuum because there are real focus points in the amplifier. Before amplification, the input Gauss beam firstly goes through a diaphragm and then a static spatial filter with a pinhole, the beam is refitted into a 4th order super-gaussian beam. Then, the image of super-gaussian beam is relayed to the first spatial filter of amplifier. The Ti:sapphire crystal is put at the surface of image or object of the spatial filters for the sake of the good qual