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1.
LD侧泵浦Nd:YAG板条双程功率放大器初步研究   总被引:6,自引:6,他引:0       下载免费PDF全文
 对二极管激光侧泵浦Nd:YAG板条双程功率放大器进行了初步的研究,给出了激光器的数值模拟结果,建立了二极管侧面泵浦Nd:YAG板条激光主振荡-多程放大(MOPA)系统;在100Hz重复频率时,实验获得单脉冲能量为51.9mJ的输出,光束质量M 2小于2,脉冲能量起伏小于2%, 实验结果与数值计算结果相符合。  相似文献   

2.
对稳定和非稳共焦型Nd:YAG板条激光器的特性作了理论分析和实验研究.证实了使用交叉棱镜腔的流动空气-水混合冷却板条激光器有高的光束质量和对棱镜失调的不灵敏性,可望获得某些实际应用.关键词:交叉棱镜腔,板条激光器.  相似文献   

3.
设计了一种高倍率的固体皮秒脉冲激光放大器,采用Nd:YAG板条作为激光增益介质。借助板条结构的角度选通结构,搭建了板条五通放大系统,实现了对注入皮秒脉冲激光的高倍率放大。种子源工作在脉冲模式,放大器泵浦源在连续模式工作。皮秒光纤激光器可以在不同的重复频率下工作,脉冲宽度为13.4 ps。种子光经过隔离和耦合系统之后,注入板条的单脉冲能量为25 nJ。当种子源工作重复频率为24.46 MHz时,板条放大器输出平均功率377 W,单脉冲能量15.5 μJ;当种子源工作重复频率为49.8 kHz时,板条放大器输出平均功率89 W,单脉冲能量1.8 mJ,峰值功率为134 MW,放大倍率达到7.2×104。  相似文献   

4.
理论设计了二极管端面抽运Nd:YAG复合陶瓷板条,制作了双浓度掺杂的Nd:YAG复合陶瓷板条。当二极管总抽运功率为18.06kW时,通过双程放大提取了7.08kW的激光功率,光光转换效率高达39.2%,单程传输的退偏振约为3.2%。实验结果表明,Nd:YAG复合陶瓷板条对提高板条激光器的输出功率和减小退偏振具有显著的效果。  相似文献   

5.
针对高平均功率固体激光器对Nd:YAG晶体板条的技术需求,进行了Nd:YAG晶体板条低透射波前误差加工技术研究。详细分析了光学加工过程中引起板条端面透射波前畸变的误差来源,并提出工艺技术解决方案。实验结果表明,在板条抛光阶段通过采用合成盘硬抛光工艺以及新的工件装夹技术,能够解决传统板条加工工艺在面形及楔角精度方面可控性差的问题,更容易实现Nd:YAG晶体板条的低透射波前误差加工。对于150mm×30mm×2.5mm规格的Nd:YAG晶体板条元件,端面透射波前畸变PV值达到0.74λ。  相似文献   

6.
针对高平均功率固体激光器对Nd:YAG晶体板条的技术需求,进行了Nd:YAG晶体板条低透射波前误差加工技术研究。详细分析了光学加工过程中引起板条端面透射波前畸变的误差来源,并提出工艺技术解决方案。实验结果表明,在板条抛光阶段通过采用合成盘硬抛光工艺以及新的工件装夹技术,能够解决传统板条加工工艺在面形及楔角精度方面可控性差的问题,更容易实现Nd:YAG晶体板条的低透射波前误差加工。对于150mm×30mm×2.5mm规格的Nd:YAG晶体板条元件,端面透射波前畸变PV值达到0.74λ。  相似文献   

7.
针对高功率板条激光器核心工作器件——板条Nd:YAG晶体的超精密加工开展研究,分析了具有特殊构型的板条Nd:YAG晶体元件的加工性能及工艺难点,提出了一种新的基于合成盘抛光的板条Nd:YAG晶体加工工艺,并对规格为100mm×30mm×3mm的板条Nd:YAG晶体进行了加工实验。实验结果表明,合成盘抛光可以很好地控制元件的塌边现象;通过磨料的优化选择,在合成盘抛光工艺中匹配合适粒度的Al2O3磨料能够实现元件的低缺陷加工,元件下盘后的全反射面平面度达0.217λ(1λ=632.8nm),端面平面度达到0.06λ,表面粗糙度达0.55nm(RMS),端面楔角精度可达2″。  相似文献   

8.
基于激光二极管抽运棒状放大器和板条放大器相结合的方式,研制了一台应用于汤姆孙散射诊断的高重复频率、高光束质量焦耳级的Nd:YAG纳秒激光器.激光器采用主振荡功率放大的结构,主要包括单纵模种子、预放大单元和能量提取单元三部分.为了获得高光束质量的激光输出,采用相位共轭技术对激光光束畸变进行补偿.在重复频率200 Hz,单纵模种子注入单脉冲能量8.23μJ的条件下,获得了1.85)的能量输出.输出激光的脉冲宽度为5.36 ns,远场光斑为1.72倍衍射极限,能量稳定性(RMS)为1.3%.  相似文献   

9.
将氙灯抽运Nd:Ce:YAG激光器作为主振荡器,一级抽运Nd:YAG放大,实现了能量为1.8 J,脉宽为8 ns,束散角为2.3 mrad,重复频率为20 Hz的激光输出,峰值功率达0.22GW.该激光器体积更小,效率更高,可靠性更强.  相似文献   

10.
将氙灯抽运Nd:Ce:YAG激光器作为主振荡器,一级抽运Nd∶YAG放大,实现了能量为1.8J,脉宽为8ns,束散角为2.3mrad,重复频率为20Hz的激光输出,峰值功率达0.22GW。该激光器体积更小,效率更高,可靠性更强。  相似文献   

11.
采用CW锁模YAG倍频激光器同步泵浦PML飞秒染料激光器,产生了平均脉宽约55fs、功率为15mW的光脉冲。文章在理论和实验上还研究了同步泵浦飞秒激光脉冲产生技术。  相似文献   

12.
 叙述了二极管面阵侧泵浦双板条耦合单横模 Q 开关激光器的研制。泵浦源为二极管面阵激光器,使用梯形波导板耦合系统,耦合效率达90%,谐振腔为凸凹腔,全反射镜的曲率半径为 3.0m的凹面镜,输出镜为曲率半径3.0m的可变反射率超高斯镜。激光器在 100Hz 重复频率下,输出单脉冲能量18.23mJ,脉宽为15.25ns,光束质量M2<1.5具有平顶分布的超高斯光束。  相似文献   

13.
The application of lasers for processing diamond has revolutionized the diamond industry and its applications in microelectronics, microelectromechanical system (MEMS) and microoptoelectromechanical system (MOEMS) technologies. The process quality can be evaluated using spectroscopic techniques. In the present investigation, four different types of Q‐switched solid‐state lasers (with different beam parameters), namely, a lamp‐pumped Nd:YAG laser operating at 1064 nm, a lamp‐pumped Nd:YAG laser operating at second harmonically generated 532 nm, a diode‐pumped Nd:YVO4 laser operating at 1064 nm and a diode‐pumped Nd:YAG laser operating at 1064 nm, have been employed for the processing of a single‐crystal, gem‐quality, natural diamond. The main objective behind the selection of these lasers with different beam parameters was to study the effect of wavelength, pulse width, pulse energy, peak power and beam quality factor (M2 factor) on various aspects of processing (such as microcracking, material loss and cut surface quality) and their relative merits and demerits. The overall weight loss of the diamond and formation of microcracks during processing have been studied for the above four cases. The characteristics of the graphite formed during processing, elemental analysis, surface morphology of the cut surface and process dynamics have been studied using micro‐Raman spectroscopy and scanning electron microscopy (SEM). We observed that laser cutting of single‐crystal diamonds used for industrial applications can be accomplished without microcracking or surface distortion using Q‐switched Nd:YAG lasers. This allows direct processing without extensive postgrinding and polishing stages. Very efficient diamond processing is possible using diode‐pumped lasers, which results in the lowest possible breakage rate, good accuracy, good surface finish and low weight loss. From the micro‐Raman and SEM studies, it is concluded that the surface quality obtained is superior when diode‐pumped Nd:YVO4 laser is used, owing to its extremely high peak power. The maximum graphite content is observed while processing with lamp‐pumped Nd:YAG laser at 532 nm. An overall comparison of all the laser sources leads to the conclusion that diode‐pumped Nd:YAG laser is a superior option for the efficient processing of natural diamond crystals. Copyright © 2006 John Wiley & Sons, Ltd.  相似文献   

14.
A diode pumped, Q-switched Nd:YAG zigzag slab laser is developed using passive conduction cooling. Flat-flat and unstable resonators are adopted in this experiment. The 150-mJ multi-mode and 100-mJ single-mode laser outputs with pulse width of 10 ns are achieved, corresponding to optical efficiencies of 19% and 13%, respectively. The experimental result demonstrates that the laser has the property of compact structure, high efficiency, reliability, and high beam quality. The design of laser has a potential application in space environment.  相似文献   

15.
用准连续60W激光二极管列阵侧面泵浦Nd:YAG板条激光器,获得3.5mJ的激光输出和峰值功率为75kW的声光调Q激光脉冲,脉冲幅度起伏小于±1%。对研究结果进行了分析。  相似文献   

16.
High peak power Nd:YAG laser pumped by 600-W diode laser stack   总被引:1,自引:0,他引:1  
The Q-switched laser with triangle slab made of Nd:YAG crystal side pumped by 600-W quasi-cw diode laser stack has been designed. The multimode (M2≈2.6) output energy of about 42 mJ was demonstrated in free running mode for110-mJ pump energy. In Q-switch experiments, the KDDP Pockels cell was placed between the slab and rear mirror in plane-plane cavity with output coupler of 84% transmission. The energy of 8 mJ in 2.1-ns pulse duration was obtained for near TEM00 output beam. For passive Q-switching by means of Cr:YAG crystal of 12.6% unsaturated transmission, the energy of 5.1 mJ in 2.5-ns pulse duration was obtained for output beam close to TEM00 mode.  相似文献   

17.
千瓦级半导体抽运的固体热容板条激光器   总被引:12,自引:0,他引:12  
报道了千瓦级激光二极管面阵抽运固体热容激光器的理论与实验研究,分别采用Nd∶YAG单板条和双板条串接的热容激光器,利用热容激光器的理论计算模型计算了在一定的工作时间内激光输出特性,并进行了实验验证。实验中采用的晶体尺寸均为59mm×40mm×4.5mm,对单板条进行抽运时平均功率大约为5.6kW,双板条串接时为11.2kW,重复频率为1kHz,占空比为20%。实验中观察了1s的工作时间内脉冲能量输出的波动情况,单板条时单脉冲能量输出最大为1.3J,在1 s后单脉冲能量输出下降到开始的70%左右,而双板条串接时单脉冲能量输出最大为2.06J,在1s后单脉冲能量输出下降到开始的50%左右,对单块晶体采用通水冷却的准热容热管理模式能有效地降低其热效应。  相似文献   

18.
二极管面阵侧泵浦Nd:YAG双板条激光器   总被引:6,自引:5,他引:1       下载免费PDF全文
叙述了二极管面阵侧泵浦双板条耦合单模模Q开关激光器的研制。泵浦源为二极管面阵激光器,使用梯形波导板耦合系统,耦合效率达90%,谐振腔为凸凹腔,全反射镜、的曲率半径为3.0m的四面镜,输出镜为曲率半径3.0m的可变反射率超高斯镜。激光器在100Hz重复频率下,输出单脉冲能量18.23mJ,脉宽为15.25us,光束质量M2<1.5具有平顶分布的超高斯光束。  相似文献   

19.
CRRFA-30L波段射频加速器   总被引:11,自引:4,他引:7       下载免费PDF全文
主要介绍CRRFA-30L波段射频加速器结构和性能,论述了热阴极射频腔注入器、束流加速系统、微波功率源和控制等结构中主要技术及其研究进展,给出了加速器输出束流参数测量与测量结果分析,达到设计应用要求。  相似文献   

20.
二极管激光侧泵浦单横模100Hz电光调Q激光器   总被引:3,自引:0,他引:3  
王卫民  吕百达 《光学学报》1997,17(10):403-1406
介绍了二极管激光侧泵浦单横模100Hz电光调Q激光器的实验结果。泵浦源为一个线阵准连续100W二极管激光器,激光工作介质为NdYAG薄梯形板条,板条与泵浦源间用柱透镜耦合,KD*P电光晶体调Q。在100Hz重复频率下,获得单脉冲能量2.37mJ,脉宽小于7ns,光束质量因子M2=1.1的1.06μm激光,光-光效率为8.5%,斜效率为18.7%。  相似文献   

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