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1.
Cr^4+:YAG的可饱和吸收特性与被动Q开关性能研究 总被引:22,自引:6,他引:16
运用速率方程计算了Cr^4+:YAG晶体的可饱和吸收特性参数,包括初始吸收系数,饱和吸收系数,饱和光强和损耗调制度,用Cr^4+:YAG对脉冲和连续Nd:YAG激光器进行了被动调Q,在脉冲Nd:YAG激光器上得到了8ns的调Q激光脉冲,在连续Nd:YAG激光器的调Q中得到了间隔和幅度抖动小于5%的输出脉冲充列。 相似文献
2.
在Nd:YAG激光器中,用单晶硅实现了被动锁模,得到了脉冲定义为28ps左右,能量为约3μJ的锁模脉冲,并对锁模机理作了初步解释。 相似文献
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自锁模Cr:LiSAF激光器的实验研究 总被引:2,自引:1,他引:1
以功率为900mW,波长为488nm的单线氩离子激光作为泵浦源,在腔内不加任何主动调制器和可饱和吸收体的情况下实现了Cr:LiSAF激光器的飞秒级自锁模运转,得到了脉冲宽度为40fs,重复频率为100MHz,平均输出功率为45mW的稳定的锁模脉冲序列。 相似文献
4.
本文描述了利用KTP晶体和腔的基波输出镜构成非线性镜实现1.08μmNd:YAP激光器的被动锁模。实验表明,这种新的锁模技术比用染料作可饱和吸收体的被动锁模技术有很多突出的优点,具有很大的发展潜力。实验测得锁模时基波1.08μm输出2.4mJ,二次谐波0.54μm输出0.5mJ(同样条件下的静态输出为2.5mJ),基波脉冲的平均脉宽为40ps。 相似文献
5.
Cr^4+:YAG调Q特性的理论和实验研究 总被引:22,自引:1,他引:21
从理论和实验两个方面研究Cr^4+:YAG的调Q特性,测量了Cr^4+:YAG调QNd^3+:YAG激光器在不同条件下脉冲能量和脉冲宽度,并与理论结果进行比较,结果显示脉冲能量的理论结果与实验结果能较发地符合,脉冲工的理论结果与实验结果变化趋势大致相一致,文中还对Cr^4+:YAG调QNd^3+:YAG激光器的其它实验现象给出定性解释。 相似文献
6.
一种连续Nd:YAG激光锁模的新技术 总被引:1,自引:0,他引:1
本文首次报道了在连续运转的Nd:YAG激光器上通过移动腔镜实现锁模的实验研究。获得平均宽度为60ps的锁模脉冲序列。文中提出了实验结果的初步解释,表明这种锁模现象是一种增强的自锁模。 相似文献
7.
采用激光二极管双向抽运并在腔内加入了半导体可饷吸收体反射镜(SESAM),实现了Cr:LiSGAF激光器的自启动、自锁模运转。得到了脉冲宽度为45fs、平均输出功率为12mW、脉冲重复频率为90MHz的稳定的锁模脉冲序列。 相似文献
8.
演示了氙灯泵浦的Nd:YAP激光器在波长1.34μm处的被动锁模,利用染料BDN-3e溶解于二甲亚砜作为可饱和吸收体,获得了波长为1.34μm的被动锁模脉冲序列输出.锁模脉冲序列的总能量达到2.2mJ,每个脉冲的平均脉宽为120ps. 相似文献
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Cr4+:YAG crystal was used as a saturable absorber in an active-passive mode-locked Nd:YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of ~0.8 ns to 2.4 ns for a single pulse was obtained by using Cr4+:YAG crystals with the different initial transmissions, and there was a shortest pulse width. The mode-locking dynamic process of Cr4+:YAG crystal was discussed to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
12.
Cr4+∶YAG crystal was used as a saturable absorber in an active-passive mode-locked Nd∶YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of ~0.8 ns to 2.4 ns for a single pulse was obtained by using Cr4+∶YAG crystals with the different initial transmissions, and there was a shortest pulse width. The mode-locking dynamic process of Cr4+∶YAG crystal was discussed to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
13.
Cr4+ : YAG crystal was used as a saturable absorber in an active–passive mode-locked Nd : YAG laser. The stable and complete mode-locked pulse train was achieved at 1064 nm. The duration of a single pulse was obtained from 0.8 to 2.4 ns by changing the Cr4+ : YAG crystal with different initial transmission, when there was the shortest pulse width. The mode-locking dynamic process of Cr4+ : YAG crystal was analyzed by the rate equations to explain the experimental result, and the effect of excited-state absorption was considered. 相似文献
14.
By using both V3+:YAG and Co:LMA saturable absorbers, an xenon-lamp-pumped doubly passively Q-switched and mode-locked (QML) Nd:YAG laser at
1.3 μm in a straight cavity is realized for the first time. The modulation depth of QML pulse has nearly reached 100%. The
experimental results shows that the doubly passively Q-switched and mode-locked (QML) laser can generate shorter Q-switch
envelope pulse with higher average peak power in comparison to the singly passively QML laser with V3+:YAG or Co:LMA saturable absorber. 相似文献
15.
Ultrashort pulses were generated in passively mode-locked Nd:YAG and Nd:GdVO4 lasers pumped by a pulsed laser diode with 10-Hz repetition rate. Stable mode-locked pulse trains were produced with the pulse width of 10 ps. The evolution of the mode-locked pulse was observed in the experiment and was discussed in detail. Comparing the pulse evolutions of Nd:YAG and Nd:GdVO4 lasers, we found that the buildup time of the steady-state mode-locking with semiconductor saturable absorber mirrors (SESAMs) was relevant to the upper-state lifetime and the emission cross-section of the gain medium. 相似文献
16.
By considering the Gaussian spatial distributions of the intracavity photon density and the initial population-inversion density, the coupled rate equations for a diode-pumped passively Q-switched and mode-locked (QML) laser with Cr4+:YAG saturable absorber are given. These coupled rate equations are solved numerically and the key parameters of an optimally coupled passively QML laser are determined for the first time. These key parameters include the parameters of the gain medium, the saturable absorber and the resonator, which can maximize the pulse energy of singly Q-switched envelope. The optimal calculations for a diode-pumped passively QML Nd:GdVO4 laser with Cr4+:YAG saturable absorber are presented to demonstrate the numerical simulation applicable. 相似文献
17.
G. Zhang S. Zhao Y. Li G. Li D. Li K. Yang T. Li K. Cheng H. Ge Y. Zhang Z. Yu 《Laser Physics》2010,20(6):1307-1311
A diode-pumped Q-switched and mode-locked (QML) Nd:LuVO4/KTP green laser with acousto-optic modulator (AOM) and Cr4+:YAG saturable absorber is presented. By inserting an AOM into the laser cavity, the stability of the QML green laser pulse with AO and Cr4+:YAG is improved, the modulation depth is increased and the pulse width of Q-switched pulse envelope is significantly compressed in comparison with that of the singly passively QML green laser with Cr4+:YAG. The experimental results show that the peak power of the doubly QML green laser pulse is much higher than that of the singly passively QML green laser pulse. 相似文献
18.
L. H. Lin B. Ouyang S. Y. Li W. Ge Y. Y. Kang S. S. Chen 《Optical and Quantum Electronics》1991,23(3):433-438
In this paper, a high power Nd:YAG laser system is described, which consists of an actively-passively mode-locked Nd:YAG laser oscillator with variable subnanosecond pulsewidths (200 ps to 1 ns), a Pockels-cell shutter and a coaxial four-pass Nd:YAG amplifier. With the oscillator operating in the colliding pulse regime, and a BDN dye film as the saturable absorber, and an acousto-optic modulator as the active modelocker, we have achieved a shot-to-shot stability of the pulse-train amplitude < ±4%. For a 0.1 mJ, 200 ps laser pulse, we obtained four-pass amplification of 7 × 102 with a pump energy of 106 J. 相似文献
19.
Passive mode locking of a Nd:YAG laser with co-doped Nd, Cr:YAG as saturable absorber 总被引:1,自引:0,他引:1 下载免费PDF全文
We demonstrate the characteristics of relatively low saturation intensity using co-doped Nd, Cr:YAG as saturable absorber for passively mode locking the Nd:YAG laser. The difference of the saturation intensity between Q-switched and mode-locked operation in co-doped Nd, Cr:YAG was only one to two orders of magnitude, while Cr:YAG was generally reported at a difference of five orders of magnitude. More than 80% mode locking modulation depth was achieved at an incident pump power of 4.4W, corresponding to an intracavity intensity of 6×10^4W/cm^2, using a 68cm long plano-concave cavity. 相似文献