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1.
An intracavity frequency-doubled vertical external cavity surface emitting laser(VECSEL)with green light is demonstrated.The fundamental frequency laser cavity consists of a distributed Bragg reflector (DBR)of the gain chip and an external mirror.A 12-mW frequency-doubled output has been reached at 540 nm with a nonlinear crystal LBO when the fundamental frequency output is 44 mW at 1080 nm.The frequency doubling efficiency is about 30%.  相似文献   

2.
Efficient continuous-wave(CW)intracavity frequency doubling of a diode-end-pumped Nd:GdVO_4 laser operating on ~4F_(3/2)-~4I_(9/2)transitions at 912 nm has been demonstrated.A symmetrical cavity with two laser rods is designed,which divides the pump power between the two laser rods,allowing for greater power scalability.An 18-mm-long BiBO crystal,cut for critical type I phase matching,is used for the intracavity frequency-doubled laser.A maximum output power of 6.2 W in the blue spectral range at 456 nm has been achieved with the pump power of 36 W.The beam quality M~2 value is 2.5 in both horizontal and vertical directions.The ellipticity of the deep blue laser is 0.98,and the power stability is better than 3.2% at the maximum output power.  相似文献   

3.
We demonstrated a diode-pumped vertical external cavity surface emitting laser with simple plane-concave cavity. When the pump power at a wavelength of 811.6 nm is 1.5 W, the maximum output power is 40.4 mW at the wavelength of 1005.8 nm. The optical-optical conversion efficiency is 2.7%. .  相似文献   

4.
We report a cesium vapor laser with fundamental mode output and a wavelength of 894 nm. The laser is pumped by a laser diode array with an external cavity of a holographic grating by using Littrow's structure. A slope efbciency of 22.4% is obtained by using a pumping source with a linewidth of 0.26 nm and 80 kPa methane as the buffer gas. The threshold pumping power is 1.56 W.  相似文献   

5.
Efficient continuous-wave (CW) intracavity frequency doubling of a diode-end-pumped Nd:GdVO4 laser operating on 4F3/2 - 4I9/2 transitions at 912 nm has been demonstrated. A symmetrical cavity with two laser rods is designed, which divides the pump power between the two laser rods, allowing for greater power scalability. An 18-mm-long BiBO crystal, cut for critical type Ⅰ phase matching, is used for the intracavity frequency-doubled laser. A maximum output power of 6.2 W in the blue spectral range at 456 nm has been achieved with the pump power of 36 W. The beam quality M2 value is 2.5 in both horizontal and vertical directions. The ellipticity of the deep blue laser is 0.98, and the power stability is better than 3.2% at the maximum output power.  相似文献   

6.
We demonstrate the generation of red light femtosecond laser pulses from an intra-cavity frequency-doubled Cr^4+ :forsterite laser. An average output power of 75 mW is obtained at the central wavelength of 647nm with a pulse width of 55 fs by inserting a 500μm-thick BBO crystal in the laser cavity. The bandwidth of the spectrum of second harmonic pulses is 9 nm, corresponding to a time-bandwidth product of 0.355.  相似文献   

7.
A flashlamp-pumped Cr:LiSAF laser system with a voltage controlled Q-switch structure in the cavity is designed. A dual-wavelength and dual-pulse tunable laser output is gained. The relation of laser output behavior with input energy is studied experimentally. The output is dual-pulsed with the energy of the 32m J/pulse producing the total output energy of 64mJ and the pulse width is about 27ns at 850nm. Then, we use one LBO crystal as the frequency doubling crystal to obtain a dual wavelength (448.1 nm and 449.15nm) and dual pulse laser. The output for one wavelength is about 10.3mJ and the line width is less than 0.02nm.  相似文献   

8.
All-Solid-State Near-Infrared and Blue Femtosecond Laser System   总被引:1,自引:0,他引:1       下载免费PDF全文
《中国物理快报》2002,19(2):203-204
We investigate an all-solid-state continuous wave(cw) green (532nm),femtosecond near-infrared (823.1nm) and blue (402nm) laser system which is pumped by a diode-laser-pumped intracavity frequency-doubled and all-self-structuring cw Nd:YVO4/KTP 532nm green laser.The cavity parameters of the Nd:YVO4/KTP laser have been optimized and the maximum 5.6W TEM00 green laser is obtained at a 22W pump power with an optical-optical conversion efficiency of 25.5%.A Ti:Sapphire laser and nonlinear second-harmonic generation by a crystal BBO is used to obtain different wavelengths.A femtosecond laser with an average output power of 300mW at 823.1nm and 73mW at 402nm is obtained when the green pump power is 2.5W.The spectral full width at half maximum are 32.3 nm and 5.1 nm,which can sustain the pulses of 22 fs and 33.3 fs,respectively.  相似文献   

9.
We report a high-power high-efficient continuous-wave (cw) diode-end-pumped Nd:YVO4 1342-nm laser with a short plane-parallel cavity and an efficient cw intracavity frequency-doubled red laser at 671 nm with a compact three-element cavity. At incident pump power of 20.6 W, a maximum output power of 7 W at 1342 nm is obtained with a slope effciency of 37.3%. By inserting a type-Ⅰ critical phase-matched LBO crystal as intracavity frequencydoubler, a cw red output as much as 2.85-W is achieved with an incident pump power of 16.9 W, inducing an optical-to-optical conversion efficiency of 16.9%. To the best of our knowledge, this is the highest output of diodepumped solid-state Nd:YVO4 red laser. During half an hour, the red output is very stable, and the instability of output power is less than 1%.  相似文献   

10.
An all-solid-state quasi-continuous-wave dispersion cavity tunable Ti:sapphire laser pumped by a laser diode pumped frequency-doubled Nd:YAG laser is reported. Using a dense flint glass prism as the dispersion element, a tuning range from 730 to 880 nm with the linewidth of 3 nm and the pulse width of 17.2ns was obtained. The maximum output power of this laser system was 5.6 W at 786.3 nm corresponding to an optical-to-optical conversion efficiency of 25.5% under the pump power of 22 W.  相似文献   

11.
We introduce a new concept for a wavelength-tunable frequency-doubled laser diode with a single control parameter. The concept is based on intracavity frequency doubling in an external resonator geometry with spatial separation of the spectral components. The use of a fan-structured periodically poled LiTaO(3) crystal permits tuning of both the fundamental and the second harmonic simultaneously with one aperture. We demonstrate tunability over more than 10 nm in the blue (480.4 to 490.6 nm) with output powers of the order of 50 nW.  相似文献   

12.
Wang Z  Yang F  Zhang G  Bo Y  Liu S  Xie S  Xu Y  Zong N  Li F  Liu B  Xu J  Peng Q  Zhang J  Cui D  Wu Y  Xu Z 《Optics letters》2012,37(12):2403-2405
We demonstrate a high-power UV 278 nm laser by fourth-harmonic generation (FHG) of a 1112 nm Nd:YAG laser in a nonlinear optical (NLO) crystal CsB3O5 (CBO) for the first time, to our best knowledge. A 30 W level diode-pumped Q-switched Nd:YAG laser at 1112 nm with beam quality factor M2=1.2 was used as the fundamental light source at a pulse width of 500 ns. With an LiB3O5 crystal, the 1112 nm laser was first frequency-doubled to 556 nm with an average output power of 13.5 W. It was then frequency doubled again in a CBO crystal to obtain the FHG output at 278 nm. The maximum average output power of the 278 nm laser is up to 1.5 W. The results demonstrated that CBO crystal is a promising NLO material for UV high-power lasers below 300 nm.  相似文献   

13.
Sakuma J  Asakawa Y  Imahoko T  Obara M 《Optics letters》2004,29(10):1096-1098
Achievement of more than 100 mW of pure continuous-wave deep-ultraviolet radiation at 213 nm has been demonstrated in an efficient all-solid-state laser system that uses two Brewster-cut CsLiB6O10 (CLBO) crystals. The first crystal is used for 266-nm generation by external resonant doubling of 532-nm radiation from a frequency-doubled Nd:YVO4 laser. Subsequent sum-frequency mixing is performed in a second CLBO crystal placed in a diode-pumped Nd:YAG laser cavity to mix the single-pass 266-nm output with circulating 1064-nm light.  相似文献   

14.
报道了LD侧面泵浦Nd∶YAG/S-KTP腔内倍频高功率660nm连续红光激光器。泵浦组件(呈三角形等间距分布)由9个20W的激光二极管组成,最大泵浦功率为180W。通过对谐振腔参数进行优化设计,用LD连续抽运3mm×65mm Nd∶YAG激光棒时,获得了波长为1319nm的基频光振荡。利用S-KTP II类临界相位匹配腔内倍频技术,当泵浦电流为22A时,获得了6.8W的连续红光激光输出,光-光转换效率为4.3%。  相似文献   

15.
王兰  金光勇  董渊  王超 《中国光学》2021,(2):329-335
为了探究提高500 nm附近激光高准确度应用的理论和技术依据,本文采用双泵浦源复合腔结合非线性和频变换,实现腔内两种波长基频光无增益竞争,可提高基频光输出功率,同时在复合腔内进行多次非线性频率变换,通过调控基频光注入功率比,使腔内光子数配比达到1∶1,从而有效提高了光-光转换效率及和频输出功率。对首次建立的理论模型进行了实验验证,分别采用Nd:YAG和Nd:YVO4作为增益介质获取946 nm和1064 nm基频光输出,LBO为和频晶体;通过双泵浦源结构实现946 nm和1064 nm基频光无增益竞争,调节注入LBO光功率,对比注入功率比不同时的和频转换效率及输出功率,最终在基频光注入功率比为1.48∶1(即腔内光子数配比为1∶1)时获得最大输出功率923 mW的501 nm青光。  相似文献   

16.
A quasi-continuous-wave intracavity frequency-doubled Nd:YAG laser which operates at 660 nm is studied.By using a flat-flat laser cavity, 2 Kr-lamps, KTP crystal and an acousto-optically Q-switch, 2-W outputpower at 660 nm is obtained. The relationship between laser cavity length and output power is analyzed.  相似文献   

17.
高效全固化263nm紫外激光脉冲的产生   总被引:5,自引:2,他引:3  
运用半导体泵浦的Nd:YLF调Q倍频激光器输出的527nm波长激光和BBO晶体直接进行了外腔谐波倍频的实验研究.采用较小的基波光束尺寸和长聚焦相结合的方法实现了高效全固化263nm紫外激光脉冲的大功率输出.基波功率为6.0W时,紫外263nm激光输出780mW,转换效率达13%,实验中还发现紫外输出光束质量很好.  相似文献   

18.
基于外腔的高效频率转换, 尤其是当系统运行在抽运不消耗近似机理下, 信号光可实现大于90%的转换, 因此无法通过信号光直接获得其到腔模频率锁定的误差信号. 本文通过对信号光调制、和频光解调的方法获得了该误差信号, 实现了双波长激光到外腔腔模的级联锁定. 实验中外部环形腔将1.3 W的1064 nm抽运光放大到约14.3 W. 当1583 nm信号光从10 μW变化到50 mW, 其到636 nm和频光的转化效率约为73%; 当从50 mW变化到295 mW时, 转换效率呈线性降低到60%, 最终获得了440 mW的636 nm激光.  相似文献   

19.
激光二极管抽运Nd∶YVO4/LBO红光激光器研究   总被引:1,自引:0,他引:1  
报道了激光二极管抽运的Nd∶YVO4晶体、LBO晶体Ⅱ类非临界相位匹配腔内倍频大功率红光激光器。通过对激光晶体热效应的考虑 ,设计了热不灵敏腔 ,采用低掺杂浓度Nd∶YVO4晶体 ,获得了 6 71nm红光的最高输出为890mW。  相似文献   

20.
We present for the first time, to the best of our knowledge, a frequency-doubled Nd:GdVO(4) laser operating in a cw on the pure three-level laser line at 880 nm. We obtained 300 mW at 440 nm for 23 W of incident pump power at 808 nm. Moreover, with a 25% output coupler we obtained a cw power of 1.9 W at the fundamental wavelength at 880 nm.  相似文献   

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