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Modeling a polarization-bistable neodymium laser with a Cr{sup}4+: YAG passive switch under the weak resonant radiation control

机译:用CR {SUP} 4 +:YAG无源开关在弱共振辐射控制下建模偏振 - 双稳态钕激光器

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Previously we reported the experimental observation [1] and theoretical simulation [2] of the drastic dependence of the state of polarisation of a neodymium laser passively Q-switched with a Cr{sup}4+:YAG crystal (see Fig. 1,a) on relative orientations in the laser cavity of the passive switch (PS) and an partial polariser (PP). It has been shown that polarisation state of the laser is governed both by relative orientations of the Cr{sup}4+:YAG PS and of the intracavity PP as well as by the energy density of a giant pulse (GP) in the switch. Complicate behavior of the polarisation state is due to an "interplay" between the PP action (which causes the linear anisotropy of the cavity) and that of the Cr{sup}4+:YAG crystal (which causes the nonlinear anisotropy of the cavity). In particular, when the cavity parameters are chosen by a suitable manner, one should observe sharp, by 90{deg}, jumps of the GP polarisation azimuth, while only slight (~1{deg}) azimutal tuning of the Cr{sup}4+:YAG crystal about the cavity axis takes place.
机译:以前我们报道了实验观察[1]和理论模拟[2]的钕激光器的偏振状态的激烈依赖性,被动Q-切换了CR {sup} 4 +:YAG晶体(参见图1,a )在被动开关(PS)的激光腔中的相对取向和部分偏振器(PP)。已经表明,激光的偏振状态通过CR {SUP} 4+:YAG PS和腔内PP的相对取向来控制,以及开关中的巨型脉冲(GP)的能量密度。偏振状态的复杂性行为是由于PP动作之间的“相互作用”(这导致腔的线性各向异性)和CR {SUP} 4+:YAG晶体(引起腔的非线性各向异性) 。特别地,当通过合适的方式选择腔参数时,一个人应该观察到夏普,×90 {deg},跳跃的GP偏振方位角跳跃,而CR {sup}只有轻微的(〜1 {deg})四倍化调整4+:关于腔轴的YAG晶体发生。

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