共查询到14条相似文献,搜索用时 125 毫秒
1.
2.
3.
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
4.
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
5.
全光纤调Q掺铒光纤激光器的脉冲研究 总被引:5,自引:3,他引:2
报道一种全光纤调Q掺铒光纤激光器,在其结构中采用带有光纤光栅的光纤环形镜作为调Q装置此调Q方案同时具有对腔内损耗进行调制和对激光输出波长选择的功能理论上分析了不同臂长差时的脉冲出现情况,与实验基本相符并对激光单脉冲产生及稳定性进行了分析讨论. 相似文献
6.
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
7.
8.
9.
在相对论激光强度下,对p偏振30 fs激光与固体Cu靶相互作用中产生的Kα射线进行了实验研究.采用刀边成像技术和单光子计数X射线CCD相结合的探测装置,在单发激光脉冲打靶时同时得到X射线源的尺寸、能谱以及Kα光子的转换效率等多种信息.实验结果与Reich等人的理论计算结果有明显的差异,Kα光子的能量转换效率在激光功率密度为1.6×1018W/cm2的条件下达到最大值7.08×10-6/sr.根据这一结果并结合蒙特卡罗程序,推断出在这一聚焦光强下激光能量转换为前向超热电子的效率约为10%. 相似文献
10.
采用氙灯泵浦新型晶体Nd:Sr5(PO4)3F,以KTP晶体腔内倍频,实现了该晶体0.5295μm绿光激光BDN染料片调Q运转。测量了输出绿光激光的特性及不同腔长和染料片小信号透过率情况下的输出能量及脉冲宽度,给出了染料片调Q腔内倍频的耦合波方程组,数值求解该方程组,所得的理论数据与实验结果较好地相符。 相似文献
11.
By taking into account turnoff time of the slowly active Q-switch, the coupled equations of a slowly actively Q-switched laser are given. These rate equations are solved numerically. The key parameters of an optimally coupled actively Q-switched laser with the turnoff time are determined, and a group of general curves are generated for the first time. These key parameters include the optimal normalized coupling parameter which maximizes the output energy, and the corresponding normalized energy, normalized peak power and normalized pulse width. The curves clearly show the dependence of the optimal key parameters on the parameters of the gain medium and the resonator. In addition, the importance of including turnoff time of the slowly active Q-switch is also shown. The optimal calculations for an actively Q-switched Nd:YVO4 laser with acoustic–optic modulator are presented to demonstrate the use of the curves and the related formulas. 相似文献
12.
13.
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
14.
P. R. Hammond 《Applied Physics A: Materials Science & Processing》1977,14(2):199-203
Loss of gain in a dye medium as a result of decomposition by pump photons is considered in terms of disappearance of dye molecules
and the appearance of a new, single chemical product having absorption in the fluorescence band. The cases of small signal
gain and saturated gain are applied to a single pass through a transversely excited amplifier. Loss of output, defined as
“quantum yield of laser deterioration”,Q
L
, is related to the true quantum yield of molecular destruction of the dye,Q
M
, and other known parameters. For the experimentally common, saturated gain condition, the smallestQ
L
can be isQ
M
, which requires a photochemically bleachable dye with high gain, preferably at high concentration, in a long cavity, operating
at high injection and pumping fluxes. Reversing these conditions, the highest valueQ
L
can be, compared withQ
M
, is unrestricted.
This work was performed under the auspices of the U.S. Energy Research and Development Administration. Contract No. W 7405
Eng 48. 相似文献