共查询到15条相似文献,搜索用时 140 毫秒
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本文从理论出发,分析抗共振环(Anti-ResonantRing-ARR)稳定调Q 激光脉冲的作用.将新型调Q晶体Cr4+:YAG置于ARR中心,在平-ARR介稳腔中获得能量起伏0.34%的高稳调Q单脉冲输出. 相似文献
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用时域ABCD矩阵对调Q锁模激光器的研究 总被引:3,自引:3,他引:0
用时域ABCD矩阵讨论了调Q锁模脉冲激光器输出脉冲的宽度和啁啾特性,主要给出了调Q元件作为幅度调制元件时的时域ABCD矩阵,并将光脉冲在激光腔中往返一周的ABCD矩阵写出,用此矩阵讨论了它对锁模脉冲的影响.给出了Nd:YAG激光器中用Cr4+:YAG作调Q元件时的调Q锁模脉冲激光器特性,并讨论了腔内色散、饱和吸收强度、增益带宽对输出脉冲特性的影响.用时域ABCD矩阵大大简化了计算过程. 相似文献
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二极管泵浦被动调Q Nd:YAG/ KTP绿光激光器 总被引:1,自引:1,他引:0
报道了LD泵浦的Nd:YAG/KTP/Cr:YAG结构被动调Q绿光激光器.当注入泵浦功率为750mW时,获得了平均功率38mW,脉冲宽度14.7ns,重复频率20.4kHz,峰值功率126.6W的调Q绿激光输出. 相似文献
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自锁模飞秒掺铬的镁橄榄石激光器的实验研究 总被引:3,自引:0,他引:3
用波长为1.06μm的Nd:YAG激光器泵浦Cr4+:forsterite晶体,实现了Cr4+:forsterite激光器的自锁模飞秒激光运转,在吸收泵浦功率为8W的条件下,得到了脉冲宽度为85fs,中心波长为1246nm,平均输出功率为200mW的稳定锁模输出。 相似文献
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基于Yb3+抽运动力学,结合光线追迹的方法,建立了抽运过程中的放大自发辐射模型,得到激光介质中三维含时储能分布.将速率方程理论和角谱传播理论结合,对谐振腔内调Q脉冲的形成、传播过程进行建模计算,得到激光脉冲的时间-空间分布和光束质量因子变化规律.同时进行了激光二极管抽运重频Yb:YAG片状激光器电光调Q实验,并与模拟计算的结果进行了对比校核,印证了计算模型的正确性.这为主动调Q固体激光器的设计提供了参考.
关键词:
Yb:YAG激光器
Q')" href="#">调Q
时空演化 相似文献
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在不同初始边界条件下数值求解描述全光纤声光调Q双包层光纤激光器的速率方程,得到前向抽运结构和后向抽运结构下激光器上能级粒子数在增益光纤中的分布,以及脉冲能量、平均功率、脉宽、光纤中储能与脉冲重复频率、抽运合束器对信号光透过率、抽运功率的相互关系.从谐振腔内放大自发辐射光的产生影响谐振腔损耗的角度分析仿真结果,并实验验证两种抽运方式对输出脉冲功率和脉冲宽度的影响.结果表明:不同脉冲重复频率下抽运方式会对全光纤声光调Q激光器性能产生显著影响,为获得较好的脉冲输出性能,在重复频率较低
关键词:
光纤激光器
Q')" href="#">声光调Q
抽运方式 相似文献
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N.D. Lai M. Brunel F. Bretenaker O. Emile 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,19(3):403-410
We study theoretically and experimentally different methods to control the pulses emitted by solid-state lasers passively
Q-switched by a saturable absorber. We explore one- and two-axis laser schemes allowing to control the pulse duration, which
is ruled by the saturation powers of the transitions in the absorber and in the gain medium. In one-axis lasers, it is shown
that the adjustment of the pump and laser beam sizes in the active medium and in the absorber provides an efficient means
to control the pulse temporal shape and duration. Furthermore, a two-axis laser cavity supporting so-called forked-eigenstate
operation permits to freely adjust the parts of the mode power which circulate in the gain medium and in the absorber. In
this case, a lengthening of the pulse duration up to 500 ns is obtained with an increase of the average output power. The
theoretical results obtained by using rate equations adapted to each cavity geometry are in close agreement with experiments
performed on a diode-pumped Nd3+:YAG laser Q-switched by a Cr4+:YAG saturable absorber. The relevance of the different techniques to control the pulse durations in the framework of potential
applications is discussed.
Received 3 December 2001 相似文献
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A compact, diode-pumped passively Q-switched Nd3+:Gd3Ga5O12 (Nd:GGG) laser with Cr4+:YAG saturable absorber has been successfully demonstrated. Stable Q-switched pulses with pulse energy of 100 ??J and high peak power of 14 kW have been obtained. The pulse width was as short as 7 ns with low repetition rate of 10 kHz. The dependence of pulse width, pulse repetition rate, pulse energy and pulse peak power on pump power have been measured respectively. Experimental results reveal that the Nd:GGG crystal with Cr4+:YAG saturable absorber is suitable for narrow pulse width and high power passively Q-switched lasers. 相似文献
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Zhenfang Peng Yufei Ma Renpeng Yan Xudong Li Ying He Xin Yu Yao Tong Lin Ge Jiang Li 《Journal of Russian Laser Research》2018,39(2):187-191
Using simultaneously both an acousto-optic (AO) modulator and a Cr4+:YAG saturable absorber in the cavity, we demonstrate for the first time the performance of a diode-pumped doubly Q-switched Nd:YAG ceramic laser. In contrast to purely acousto-optic Q-switched laser, this doubly Q-switched laser can generate shorter and more symmetric pulses. At an absorbed pump power of 10 W and a repetition rate of 20 kHz, the pulse width is compressed to 30 and 25 ns, respectively. 相似文献