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Cavity length dependence of mode beating in passively Q-switched Nd-solid state lasers

机译:被动调Q Nd固态激光器中模式跳动的腔长依赖性

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The temporal intensity profile of pulse(s) from passively Q-switched and passively Q-switched mode locked (QSML) solid-state lasers is known to be dependent on cavity length. In this work, the pulse width, modulation depth, and beat frequencies of a Nd:Cr:GSGG laser using a Cr~(+4):YAG passive Q-switch are investigated as function cavity length. Measured temporal widths are linearly correlated with cavity length but generally 3-5 ns larger than theoretical predictions. Some cavity lengths exhibit pulse profiles with no modulation while other lengths exhibit complete amplitude modulation. The observed beat frequencies at certain cavity lengths cannot be accounted for with passively QSML models in which the pulse train repetition rate is τ_(RT)~(-1), τ_(RT)= round-trip time. They can be explained, however, by including coupled cavity mode-locking effects. A theoretical model developed for a two section coupled cavity semiconductor laser is adapted to a solid-state laser to interpret measured beat frequencies. We also numerically evaluate the temporal criterion required to achieve temporally smooth Q-switched pulses, versus cavity length and pump rate. We show that in flash lamp pumped systems, the difference in buildup time between longitudinal modes is largely dependent on the pump rate. In applications where short pulse delay is important, the pumping rate may limit the ability to achieve temporally smooth pulses in passively Q-switched lasers. Simulations support trends in experimental data. Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the U.S. Department of Energy's National Nuclear Security Administration under contract DE-AC04-94AL85000.
机译:已知来自被动Q开关和被动Q开关锁模(QSML)固态激光器的脉冲的时间强度分布取决于腔体长度。在这项工作中,研究了使用Cr〜(+4):YAG无源Q开关的Nd:Cr:GSGG激光器的脉冲宽度,调制深度和拍频,作为功能腔长。测得的时间宽度与腔体长度线性相关,但通常比理论预测值大3-5 ns。一些腔体长度表现出没有调制的脉冲轮廓,而其他腔体长度表现出完全的幅度调制。被动腔QSML模型无法解释在特定腔长处观察到的拍频,在被动QSML模型中,脉冲串的重复率为τ_(RT)〜(-1),τ_(RT)=往返时间。但是,可以通过包括耦合腔锁模效应来解释它们。为两部分耦合腔半导体激光器开发的理论模型适用于固态激光器,以解释测得的拍频。我们还从数值上评估了实现时间平滑Q开关脉冲所需的时间标准,以及腔长和泵速。我们表明,在闪光灯泵浦系统中,纵向模式之间建立时间的差异很大程度上取决于泵浦速率。在短脉冲延迟很重要的应用中,泵浦速率可能会限制在被动调Q激光器中获得时间上平滑的脉冲的能力。模拟支持实验数据的趋势。桑迪亚国家实验室(Sandia National Laboratories)是由洛克希德·马丁公司(Lockheed Martin Corporation)的全资子公司桑迪亚公司(Sandia Corporation)管理和运营的多程序实验室,根据合同DE-AC04-94AL85000为美国能源部国家核安全局管理。

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