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The phase locking control of the multichannel holographic neodymium laser system with the help of a passive Q-switch

机译:借助无源Q开关对多通道全息钕激光系统进行锁相控制

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The phase locking of laser generators requires compensation of the distortions of laser emission and the difference in the lengths of resonators. In [1–3], we suggested to phase the diffraction coupled loop laser resonators [4, 5] that provide the self compensation of the lengths and optical distortions with the phase configuration (PC) on the holographic gain gratings and experimentally produced the phased two channel and three channel holographic YAG : Nd laser systems with long range and shortrange coupling. The laser system with long range coupling (each channel with each one) provides a high interference contrast of emission of laser channels up to 0.9 [2]. However, it has limitations for an increase in the number of laser channels because of their optical coupling in one common active element. On the contrary, in the scheme with short range coupling (coupling of neighboring channels), unlimited scaling of the number of laser channels can be realized since each pair of neighboring channels has its own coupling active element. However, the interference contrast of the two channel YAG : Nd laser system operating by such scheme in a free running mode was no higher than 0.6 [3].
机译:激光发生器的锁相需要补偿激光发射的畸变和谐振器长度的差异。在[1-3]中,我们建议对衍射耦合环形激光谐振器进行相位调整[4、5],以全息增益光栅上的相位配置(PC)对长度和光学畸变进行自我补偿,并通过实验产生相位具有长距离和短距离耦合的两通道和三通道全息YAG:Nd激光系统。具有长距离耦合的激光系统(每个通道各一个)提供高达0.9 [2]的激光通道发射的高干涉对比。但是,由于激光通道在一个共同的有源元件中的光耦合,因此增加了激光通道的数量。相反,在具有短程耦合(相邻信道的耦合)的方案中,由于每对相邻信道具有其自己的耦合有源元件,因此可以实现激光信道数量的无限缩放。然而,以这种方式在自由运行模式下运行的两通道YAG:Nd激光系统的干涉对比度不高于0.6 [3]。

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