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1.
A continuous-wave(CW) 457 nm blue laser operating at the power of 4.2 W is demonstrated by using a fiber coupled laser diode module pumped Nd:YVO4 and using LBO as the intra-cavity SHG crystal.With the optimization of laser cavity and crystal parameters,the laser operates at a very high efficiency.When the pumping power is about 31 W,the output at 457 nm reaches 4.2 W,and the optical to optical conversion efficiency is about 13.5% accordingly.The stability of the output power is better than 1.2% for 8 h continuously working.  相似文献   

2.
We reported an efficient diode pumped Nd : YVO4 1 064 nm laser passively mode-locked and Qswitched by a semiconductor saturable absorber mirror(SESAM). At the incident pump power of 7. 5 W, 2.81 W average output power was obtained during stable CW mode locking with a repetition rate of 111 MHz. The optical conversion efficiency was 37.5%, and the slope efficiency was 39%. So far as we know, this is the highest optical-optical conversion efficiency with a SESAM at home.  相似文献   

3.
We reported an efficient diode pumped Nd∶YVO4 1 064 nm laser passively mode-locked and Q-switched by a semiconductor saturable absorber mirror(SESAM). At the incident pump power of 7.5 W, 2.81 W average output power was obtained during stable CW mode locking with a repetition rate of 111 MHz. The optical conversion efficiency was 37.5%, and the slope efficiency was 39%. So far as we know, this is the highest optical-optical conversion efficiency with a SESAM at home.  相似文献   

4.
A passively Q-switched mode-locked Nd:GdYVO4 laser is successfully demonstrated by using a piece of GaAs crystal grown at low temperature as the passively saturated absorber and the output coupler. Fundamental properties of the Nd: GdYVO4 laser are investigated. The maximum average output power of 3.5 W is obtained by using plainsphere when the incident pumping power is 10 W,which corresponds to an optical-optical coversion efficiency of 35%. The threshold power for the Q-switching mode-locked is 1.2 W. The maximum average output power of 1.72 W is obtained by using GaAs when the incident pumping power is 10 W,mode-locked pulse train with a repetition rate of ~113 MHz is achieved. At the incident laser pumping power of 7 W,the modulation depth is 100%.  相似文献   

5.
A continuous-wave (CW) 457 nm blue laser operating at the power of 4.2 W is demonstrated by using a fiber coupled laser diode module pumped Nd: YVO4 and using LBO as the intra-cavity SHG crystal. With the optimization of laser cavity and crystal parameters, the laser operates at a very high efficiency. When the pumping power is about 31 W, the output at 457 nm reaches 4.2 W, and the optical to optical conversion efficiency is about 13.5% accordingly. The stability of the output power is better than 1.2% for 8 h continuously working.  相似文献   

6.
Different material-doped Raman fiber lasers with very high efficiency operatingin continuous-wave are presented. With 1 W Nd :YVO4 laser pumping at wavelength of 1342 nm,single mode output power of above 500 mW (optical-to-optical conversion efficiency of 50%) is simulated in the range of 1 400-1500 nm. Using high-germanium,phosphate and high- borate silicate fibers as the gain medium, laser output at wavelengths of 1 420,1450,1480 and 1495 nm can be achieved with different geometries, which are just as pumping C-band and L-band distributed Raman fiber amplifiers.  相似文献   

7.
We report for the first time, to our knowledge, the diode-pumped continuous-wave (CW) thin-disk Yba+-doped Lu203 (Yb:LO) laser at 1 034 nm and the second-harmonic generation at 517 nm. With a 6.3% output coupler, the maximum output power is 1.17 W under a pump power of 18.5 W. Moreover, the intracavity second-harmonic generation (SHG) is also -achieved with power of 193 mW at 517 nm by using an LiB305 (LBO) nonlinear crystal. The beam quality fac- tor M2 is about 1.28. The fluctuation of the output power is about 3% in 1 h.  相似文献   

8.
A passively Q-switched mode-locked Nd:GdYVO4 laser is successfully demonstrated by using a piece of GaAs crystal grown at low temperature as the passively saturated absorber and the output coupler. Fundamental properties of the Nd: GdYVO4 laser are investigated. The maximum average output power of 3.5 W is obtained by using plainsphere when the incident pumping power is 10 W, which corresponds to an optical-optical coversion efficiency of 35%. The threshold power for the Q-switching mode-locked is 1.2 W. The maximum average output power of 1.72 W is obtained by using GaAs when the incident pumping power is 10 W, mode-locked pulse train with a repetition rate of - 113 MHz is achieved. At the incident laser pumping power of 7 W, the modulation depth is 100%.  相似文献   

9.
A diode-pumped doubly Q-switched Nd∶YAG laser operating at 1064nm both with an acoustic-optical(AO)modulator and Cr4+∶YAG saturable absorber in the cavity is demonstrated.At the incident pump power of 11.8W the laser can generate stable 8ns pulse with the peak power of 23.6kW at a 10kHz repetition rate.The pulse temporal profile is more symmetric and shorter compared with that of passively Q-switched lasers with only AO-active and Cr4+∶YAG.A reasonable analysis is developed to explain the experimental resul...  相似文献   

10.
An all-solid-state Pr:KY3F10(Pr:KYF) laser pumped by blue laser(471 nm) has been demonstrated.With the incident pump power of 2.6 W,the maximum output power at 610 nm is 213 mW.Moreover,the intracavity second-harmonic generation(SHG) is also achieved with the maximum ultraviolet(UV) power at 305 nm of 11 mW by using a β-BaB2O4(BBO) nonlinear crystal.  相似文献   

11.
3.6W全固态腔内和频Nd∶YVO4橙黄激光器   总被引:1,自引:1,他引:0  
报道了一种采用光纤耦合激光二极管阵列(LDA)端面泵浦Nd∶YVO4激光晶体、Ⅰ类临界位相匹配BiB3O6(BiBO)腔内和频实现全固态连续橙黄色激光输出的实验结果。波长为593.5 nm的橙黄色激光是由Nd∶YVO4晶体1064 nm和1342 nm双波长非线性和频产生的。当泵浦功率为27.5 W时,得到橙黄色激光最大输出功率3.6 W,光-光转换效率高达13.2%,据我们所知,这是目前利用腔内和频Nd∶YVO4激光器获得593.5 nm橙黄色激光输出的最高效率。  相似文献   

12.
报道了一种利用复合腔进行腔内和频的589nm激光器.激光器由两个子谐振腔组成.在两个子谐振腔中,分别利用两个激光二极管(LD)抽运Nd∶YAG晶体和Nd∶YVO4晶体,并分别选择1319 nm波长(对应Nd∶YAG晶体的4F3/2→4I13/2跃迁)与1064 nm波长(对应Nd∶YVO4晶体的4F3/2→4I11/2跃迁)振荡进行和频.通过谐振腔的优化设计,实现了腔内两个波长较好的模式与增益匹配.在两个子腔的交叠部分,利用BiB3O6(BIBO)晶体Ⅰ类临界相位匹配进行腔内和频,得到和频激光输出.当Nd∶YAG与Nd∶YVO4晶体上抽运功率分别为750 mW和600 mW时,获得了24 mW,589 nm黄橙激光输出.该输出激光光束质量好、噪声低.  相似文献   

13.
LD抽运Nd:YVO_4腔内倍频连续波8.8W绿光激光器   总被引:22,自引:5,他引:17  
报道了用 LD双向抽运 Nd:YVO4晶体 ,KTP作腔内倍频的大功率绿光激光器。通过对大功率抽运情况下所产生的热透镜效应进行分析和估算 ,优化了热稳腔参数 ,获得了较稳定的功率输出。在抽运功率为 2 8W时 ,获得最大连续波绿光输出 8.8W,光 -光转换效率达 31 .5%。  相似文献   

14.
报道了全固态连续波613nm橙光激光器,橙激光是分别由Nd:YAG和Nd:YVO4晶体的1444nm和1064nm谱线非线性和频产生的,两条谱线在各自晶体对应能级跃迁分别为4F3/2-4I13/2和4F3/2-4I11/2.实验中采用复合腔结构,利用KTP晶体Ⅱ类临界相位进行内腔和频,当注入到Nd:YAG和Nd:YVO4晶体的泵浦功率分别为20W和10W时,获得344mW的TEM00连续波613nm橙激光输出.4h功率稳定度优于±2.8%.  相似文献   

15.
报道了一种光纤耦合半导体激光二极管(LD)阵列端面抽运Nd∶YVO4晶体,腔内Ⅰ类临界相位匹配LBO(LiB3O5)晶体倍频,实现波长为671nm的全固态红光激光器瓦级连续输出的理论分析和实验结果.采用短三镜折叠腔结构,通过对激光晶体热效应的考虑,估算其热透镜焦距,用计算机优化设计选取合适谐振腔参数,在26W的注入泵浦功率下,获得了连续输出6.8W、波长为671nm的红光基模稳定输出,光-光转化效率达到26%.  相似文献   

16.
全固态高输出功率单频Nd:YVO4/KTP激光器   总被引:1,自引:2,他引:1  
利用光纤耦合输出的半导体激光器(LD)端面抽运Nd∶YVO4晶体,激光谐振腔采用四镜环形腔结构,通过KTP晶体内腔倍频,获得了高功率全固态连续单频绿光激光输出。根据临界相位匹配下椭圆高斯光束的倍频理论,通过旋转Nd∶YVO4晶体的方向选取合适的基频光偏振方向,使KTP晶体的走离角所在平面与谐振腔弧矢面平行,可提高内腔倍频转换效率。当抽运功率为20 W时,激光器最大单频绿光输出功率达4.8 W。作为对比,控制基频光偏振方向使KTP晶体的走离角所在平面与谐振腔子午面平行时,激光器最大单频绿光输出功率为4.1 W。对比两种情形下的实验结果,激光器的光-光转换效率从21.8%提高到25.5%。  相似文献   

17.
报道了全固态连续波554.9nm黄光激光器,黄激光是分别由Nd:YAG和Nd:YVO4晶体的1342nm和946nm谱线非线性和频产生,两条谱线在各自晶体对应能级跃迁分别为^4F3/2-^4I11/2和^4F3/2-^4I9/2。实验中采用复合折叠腔结构,利用LBO晶体I类临界相位进行内腔和频,当注入到Nd:YAG和Nd:YVO4晶体的泵浦功率分别为20W和8W时,获得850mW的TEMoo连续波554.9nm黄激光输出。4小时功率稳定度优于±2.5%.  相似文献   

18.
介绍了一种光纤耦合激光二极管阵列(LDA)同时泵浦Nd:YAG和Nd:YVO4晶体输出554.8nm连续波的全固态黄-绿光激光器。黄-绿激光是由Nd:YAG晶体的946nm激光和Nd:YVO4晶体的1342nm激光非线性和频产生,两条谱线在各自晶体的对应能级跃迁分别为4F3/2-4I9/2和4F3/2-4I13/2。实验中采用复合腔结构,利用KTP晶体II类临界相位匹配进行腔内和频,当注入到Nd:YAG和Nd:YVO4晶体的泵浦功率分别为30W和20W时,获得了1.13W的连续波554.8nm黄-绿激光输出,光束质量因子M2<1.22,这是目前为止该波长已见报道的最高功率输出值。实验结果表明:采用Nd∶YAG和Nd∶YVO4两种激光晶体进行腔内和频是获得黄-绿激光的高效方法,并可以应用到其他两种激光晶体进行腔内非线性和频,获得更多不同波长的激光输出。  相似文献   

19.
付林  李斌 《红外与激光工程》2012,41(8):2038-2041
报道了一种单LD泵浦Nd:YVO4双晶体腔内和频实现黄光激光的有效方法,并对其进行了理论分析、实验装置的设计和实验验证。该装置由半导体激光器、光学耦合系统(CO)、Nd:YVO4镀膜晶体、镀高反膜的平凹镜、镀增透膜的LBO、镀高透膜的全反镜组成。实验采用V型谐振腔,在中心波长为808.7 nm、5 W抽运功率下,利用Ⅰ类临界相位匹配LBO作为和频晶体,获得了244 mW、593 nm的黄光输出,光-光转换率为4.9%,激光不稳定度为5%。实验结果表明:采用V型谐振腔进行腔内和频,可以获得593 nm的黄光激光,并且结构紧凑、转换效率高,可以应用到很多种和频激光器中。  相似文献   

20.
激光二极管抽运Nd:YVO4晶体五倍频213 nm深紫外激光器   总被引:2,自引:0,他引:2  
报道了一种声光调Q激光二极管抽运Nd:YVO4晶体腔外五倍频213nm深紫外全固态激光器。实验上分别利用KTP和两块BBO晶体产生532nm倍频绿光,266nm紫外四倍频以及基波与四倍频的混频,实现了从Nd:YVO4近红外激光到213nm深紫外激光的频率变换。在10.3W抽运功率下,获得平均输出功率3.1mW,脉宽7.5ns的213nm深紫外激光输出。  相似文献   

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