共查询到19条相似文献,搜索用时 125 毫秒
1.
BBO晶体在CPM非稳腔Nd:YAG激光器中的腔内倍频效应 总被引:1,自引:1,他引:0
本文报道用BBO晶体作为腔内倍频元件,在带抗共振环的对撞脉冲锁模非稳腔Nd:YAG激光器中实现腔内倍频激光输出,获得倍频能量转换效率为50.4%.理论和实验均证明了该激光器的BBO腔内倍频转换效率高于腔外倍频转换效率. 相似文献
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共焦非稳腔中ps激光的内腔倍频 总被引:2,自引:1,他引:1
考虑倍频晶体相位匹配接收角(Angular acceptance)对倍频转换效率的影响,设计了正支(p支)共焦非稳腔Nd:YAP锁模激光器。平行光通过晶体实现完全相位匹配。以BBO和KTP作为腔内倍频元件,分别获得80.6%和60.2%的高效倍频转换,及几十mJ的绿光输出。同时实验测定其它有关参数。 相似文献
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皮秒激光瞬态受激光喇曼散射的实验研究 总被引:1,自引:1,他引:0
本文采用对撞脉冲锁模Nd:YAG激光器输出10ps脉冲串,经KTP非线性晶体腔外倍频,泵浦喇曼介质为二甲亚砜(DMSO)液体。实验研究了不同透镜焦长,焦点位置不及不同喇曼介质长度对瞬态受激喇曼散射的影响,获得了能量转换效率分别为45.6%和10.5%的前,后和同阶斯托克斯-喇曼射光,,并以实验结果进行了讨论。 相似文献
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由变反镜耦合输出的卡塞格林非稳腔激光技术研究 总被引:2,自引:1,他引:1
讨论了变反镜参数和由变反镜耦合输出的卡塞格林非稳腔参数的相互关系以及它们对激光光束特性的影响。在此理论基础上,设计了Nd:YAGQ形状高功率高光束质量的激光系统,获得了脉冲能量为1.4JEM00模,脉宽10ns,重复频率10pps,束散度达到衍射极限的1.1倍,其倍频效率及混频效率分别为60%和30%。 相似文献
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本文描述我们设计的带抗共振环 (ARR)的对撞脉冲锁模 (CPM )非稳腔Nd :YAP和Nd :YAG激光器 ,该激光腔结合了CPM腔脉宽窄、工作稳定和非稳腔输出能量高的特点 ,是一理想的高功率激光器 同时选择了KTP、BBO和LBO等优良非线性晶体作为腔内倍频元件 ,实现高效倍频转换 获得× 1 0mJ和 5GW /cm2 的高能量和高功率绿光皮秒脉冲输出 ,倍频转换效率高达 ( 50~ 70 ) % 相似文献
6.
本文描述我们设计的带抗共振环(ARR)的对撞脉冲锁模(CPM)非稳腔Nd:YAP和Nd:YAG激光器,该激光腔结合了CPM腔脉宽窄、工作稳定和非稳腔输出能量高的特点,是一理想的高功率激光器同时选择了KTP、BBO和LBO等优良非线性晶体作为腔内倍频元件,实现高效倍频转换获得×10mJ和5GW/cm2的高能量和高功率绿光皮秒脉冲输出,倍频转换效率高达(50~70)%. 相似文献
7.
利用对撞脉冲锁模非稳腔Nd:YAG激光器,采用KTP非线性晶体作腔外倍频,结合受激拉曼散射技术,在一台锁模激光器同时得到1.06μm,0.53μm,0.63μm超短光脉冲的输出。 相似文献
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采用光谱物理公司生产的,平均输出工为1.1W,脉宽为90fs的再生锁模掺钛蓝宝石(Ti:Sapphire)激光器作为泵浦源,KTP作为非线性光学介质,以及BBO作为腔内倍频晶体,制成了一台同上泵浦腔内倍频飞秒KTP光学参量振荡器,其输出调谐范围528nm至586nm,最佳平均输出功率为240mW左右,脉宽约为100fs。在无反馈伺服系统的情况下,该参量振荡器可维持振荡达三个小时。 相似文献
11.
WU Fengtie 《Chinese Journal of Lasers》1994,3(2):97-103
Intracavityfrequencydoublingeffectsofpassivelymode-lockedNd:YAPpulsedlaserintwodifferentunstableresonatorsWUFengtie(Departmen... 相似文献
12.
为了增大皮秒注入种子激光的能量,获得较高的激光放大效率和信噪比,关键是要在保持较高的平均锁模激光功率下实现连续波锁模激光器的低重复频率运转。通过选取五镜折叠激光谐振腔腔型和参数设计,克服了随着腔长增加损耗加大而导致的激光锁模不稳定的困难。分析了较长腔长条件下工作物质和SESAM光斑尺寸的大小和变化,及其对激光器稳定性的影响。由于SESAM饱和工作和稳态条件的能量要求,在激光谐振腔调整过程中,对应臂长的光程互补变化。实验中采取腔长和晶体热控制方式,优化了激光谐振腔的工作参数,实现了脉冲能量10.7 nJ,重复频率56 MHz,平均功率1.2 W的SESAM连续波锁模激光输出。 相似文献
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An energy conversion efficiency of 65.3% for second harmonic generation (SHG) from 1.06 μm to 0.53 μ m has been achieved by intracavity frequency doubling (IFD) in LiB 3O 5(LBO) crystal and a colliding pulse mode locked (CPM) Nd:YAG pulsed laser with a convex antiresonant ring (ARR) unstable resonator. For a fundamental wave with 20.2 mJ energy, 10 ps duration and a energy stability of 96.4%, a green output energy of 13.2 mJ was obtained. The energy conversion efficiency in IFD is much higher than that in extracavity frequency doubling (EFD) which is only 33.87%. 相似文献
14.
G.C. Reali 《Optics Communications》1980,35(2):264-266
Experimental results on mode-locked action of a polarization coupled unstable resonator YAG laser are reported. The main features of this oscillator are ~ 20 mJ per pulse, good spatial profile and high focusable energy. 相似文献
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Cr^4+:YAG在对撞脉冲锁模的Nd:YAG激光器中实现被动锁模的研究 总被引:8,自引:1,他引:7
在理论上提出了Cr^4+:YAG作为可饱和吸收体在Nd:YAG激光器中实现被动锁模的可能性,运用速率方程组导出在强激光脉冲作用下Cr^4+:YAG激发态吸收的恢复时间和饱和光强。实验上在带有抗共振环结构的接近于介稳腔的脉冲式Nd:YAG激光器中用Cr^4+:YAG作为可饱和吸收体实现被动锁模运转,得到能量13.5mJ、平均脉宽180ps的锁模脉冲序列。 相似文献
16.
We report direct generation of 81 nJ chirped pulses from a room-temperature, Kerr lens mode-locked Cr??:forsterite oscillator operating at 1258 nm. To increase the pulse energy, the pulse repetition rate of the short x-type resonator was lowered from 143 to 4.9 MHz by the addition of a q-preserving multipass cavity, which provided an additional effective optical path length of 59.4 m. The duration of the chirped pulses was around 5.5 ps with a spectral width of 21 nm. The pulses were externally compressed to 607 fs by using a diffraction grating pair. To our knowledge, this is the highest reported pulse energy directly generated from a room-temperature mode-locked Cr??:forsterite laser. 相似文献
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C. Theobald M. Weitz R. Knappe R. Wallenstein J.A. L’huillier 《Applied physics. B, Lasers and optics》2008,92(1):1-3
This paper reports on a passively mode-locked and Q-switched Nd:YVO4 laser generating picosecond pulses with an average output power exceeding 7 W. In a first step Q-switch mode-locking was
obtained by self Q-switching of a mode-locked oscillator with appropriate cavity design, pump power and output coupling. In
a second system the Q-switching was actively controlled and stabilized by modulating the resonator internal losses with an
acousto-optic modulator. In the Q-switch mode-locking operation the laser provided 12.8 ps long mode-locked pulses with a
repetition rate of 80 MHz. The repetition rate of the Q-switch envelope was 185 kHz. The maximum pulse energy of a single
ps pulse was 0.55 μJ which is 5.5 times the pulse energy measured for cw mode locking. The total energy of the pulses within
the Q-switch envelope was 42 μJ.
PACS 42.55.Xi; 42.60.Fc; 42.60.Gd 相似文献
19.
An optical pulse narrowing technique by spectral windowing using a Fabry-Perot resonator is demonstrated. A 150 ps pulse from a mode-locked Ar ion laser has been compressed by a factor of 2.7. 相似文献