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晶体热效应对LD端面泵浦固体激光器优化设计的影响 总被引:23,自引:12,他引:11
考虑了激光介质因受热不均匀而引起的热效应对激光器衍射损耗和谐振腔基模尺寸的影响,利用M2因子来描述泵浦光在激光介质中的传播规律,根据泵浦光在激光介质中的有效泵浦体积最小以提高泵浦效率这一判据,给出了含有泵浦光束质量因子Mp2和激光介质参量在内的端面泵浦固体激光器的优化设计曲线,利用这些曲线可方便地指导完成激光器的最佳化参量选择.利用上述理论,对LD端面泵浦光纤耦合输出的Nd:YVO4激光器进行了研究,实验结果和理论分析相符合. 相似文献
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新型Nd^3+:Ca4GdO(BO3)3自倍频晶体Cr^4+:YAG被动调Q激光特性研究 总被引:2,自引:0,他引:2
采用氙灯抽运自倍频晶体Nd^3 :Ga4GdO(BO3)3(简称Nd:GdCOB),Cr^4 :YAG被动调Q,实现了Nd:GdCOB晶体被动调Q激光运转,测量了饱和吸收体Cr^4 :YAG不同小信号透过率小绿激光单脉冲的输出能量、脉冲宽度、重复率,给出了描述Nd:GdCOB晶体调Q工作原理的耦合波方程组,数值求解了该方程组,所得的理论结果与实验值相符合。 相似文献
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The intracavity photon density is assumed to be of Gaussian spatial distributions and its longitudinal variation is also considered in the rate equations for a laser diode(LD)end-pumped passively Q-switched Nd:YVO4 laser with GaAs saturable absorber.These space-dependent rate equations are solved numerically.The dependences of pulse width,pulse repetition rate,single-pulse energy,and peak power on incident pump power are obtained.In the experiment,the LD end-pumped passively Q-switched Nd:YVO4 laser with GaAs saturable absorber is realized and the experimental results are consistent with the numerical solutions. 相似文献
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偏振模色散动态补偿中色度色散影响的研究 总被引:2,自引:0,他引:2
分析了色度色散(CD)对偏振模色散(PMD)动态补偿中偏振度(DOP)反馈的影响,模拟和实验验证了2.5Gb/s和10Gb/s非归零调制系统中光信号偏振度特性和系统误码率特性。表明有色度色散作用时信号偏振度值比仅受偏振模色散作用时要大.但误码率随色度色散量增加先轻度好转后就逐渐变差.偏振度值将不能如实反映偏振模色散对系统性能的影响。且信号两正交偏振分量间能量差别越小或差分群延迟越大,上述两种情况下信号偏振度值偏离就越远。这种偏离还随系统速率和色度色散量的增加而加剧。进一步探讨了实际偏振模色散补偿中减轻色度色散影响的措施,表明当系统中同时存在偏振模色散和色度色散影响时,必须在基于偏振度反馈的偏振模色散补偿前完成色度色散补偿。 相似文献
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Gold nanorods(GNRs) with two different aspect ratios were successfully utilized as saturable absorbers(SAs) in a passively Q-switched neodymium-doped lutetium lithium fluoride(Nd:LLF) laser emitting at 1.34 μm. Based on the GNRs with an aspect ratio of five, a maximum output power of 1.432 W was achieved, and the narrowest pulse width was 328 ns with a repetition rate of 200 kHz. But, in the case of the GNRs with the aspect ratio of eight, a maximum output power of 1.247 W was achieved, and the narrowest pulse width was 271 ns with a repetition rate of 218 kHz. Our experimental results reveal that the aspect ratios of GNRs have different saturable absorption effects at a specific wavelength. In other words, for passively Q-switched lasers at a given wavelength, we are able to select the most suitable GNRs as an SA by changing their aspect ratio. 相似文献
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