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1.
A diode-bar side-pumped YAG/Nd:YAG/YAG composite crystal laser is presented. A maximum output power of 18.4 W at 1.064 μm with a slop efficiency of 57% and an optical-optical conversion efficiency of 46% was obtained for a pump power of 40 W. Compared with a side-pumped conventional crystal laser in the same experimental conditions, the side-pumped composite crystal laser improved the optical-to-optical conversion efficiency by 12%. Experimental results indicate that a composite crystal can depress the thermal effects effectively and improve the optical-to-optical conversion efficiency easily in the diode side-pumped lasers. The composite crystal has great potential in high-power diode side-pumped lasers.  相似文献   

2.
Diode-pumped 10 W continuous wave cesium laser   总被引:1,自引:0,他引:1  
Zhdanov B  Knize RJ 《Optics letters》2007,32(15):2167-2169
An efficient cesium vapor laser pumped with a continuous wave laser diode array has been demonstrated. The linewidth of the pump source was narrowed using the external cavity to match it to the cesium absorption line. The output power of the continuous wave cesium laser was 10 W, which exceeds previous results by more than a factor of 10, and the slope efficiency was 68%. The overall optical efficiency was 62%, which is a factor of 6 higher than previous pulsed laser results for alkali lasers with diode laser array pumping.  相似文献   

3.
A close-coupled scheme has been developed to end-pump the Nd:YAG rod using diode lasers tuned to 808 nm. By using a single diode laser, an optical-to-optical conversion efficiency of about 40% has been demonstrated in the multimode operation at 1064 nm.  相似文献   

4.
樊莉  赵伟倩  乔鑫  夏长权  汪丽春  范会博  沈明亚 《中国物理 B》2016,25(11):114207-114207
We report an efficient continuous-wave self-Raman laser at 1176 nm based on a 20-mm-long composite YVO_4/Nd:YVO_4/YVO_4 crystal and pumped by a wavelength-locked 878.9 nm diode laser.A maximum output power of 5.3 W is achieved at a pump power of 26 W,corresponding to an optical conversion efficiency of 20%and a slope efficiency of 21%.The Raman threshold for the diode pump power was only 0.92 W.The results reveal that in-band pumping by a wavelength-locked diode laser significantly enhances output power and efficiency of self-Raman lasers by virtue of improved pump absorption and relieved thermal loading.  相似文献   

5.
二极管泵浦无机液体激光器出光实验研究   总被引:4,自引:2,他引:4       下载免费PDF全文
 为探索新的高能激光体系,搭建了二极管泵浦的液体激光器。采用激光二极管作为泵浦光源,单侧泵浦掺钕离子的无机激光液体,进行了出光实验。通过测量输出光束的近场分布、脉冲波形和光谱,证实实现了激光输出,输出激光的波长为1 053 nm。输出的单脉冲激光能量达到47 mJ,光-光转换效率达到14%。其光-光转换效率高出闪光灯泵浦液体条件下2个数量级,说明该激光体系具有向高能激光体系发展的前景。  相似文献   

6.
Side-pumped fiber laser   总被引:1,自引:0,他引:1  
A neodymium-doped side-pumped double-clad fiber laser operating at 1.06 µm is described. We report here, what is, to our knowledge, the first exclusively repetitive side-pumping scheme with two monomode laser diodes. Side-pumping has been realized by prism-fiber couplers. A pump-light-loss analysis at the pump positions has been performed. An output power of 13.5 mW is obtained with both diode lasers. The highest slope efficiency of 66% with respect to absorbed pump power at 809 nm is achieved when pumping with only one diode.  相似文献   

7.
Schellhorn M  Hirth A  Kieleck C 《Optics letters》2003,28(20):1933-1935
We report a compact Ho:YAG laser that is intracavity pumped by a diode-pumped Tm:YLF laser. Both lasers exhibit pulse mode behavior. Operating both crystals at room temperature (25 degrees C), we obtained 1.6 W of average output at 2.09 microm from the Ho:YAG laser for 15.4 W of diode power incident upon the Tm:YLF rod and a slope efficiency of 21%.  相似文献   

8.
28% electrical-efficiency operation of a diode-side-pumped Nd:YAG rod laser   总被引:3,自引:0,他引:3  
We propose a highly efficient quasi-cw Nd:YAG rod laser with a novel side-pumping design that uses microlens-free diode stacks. We demonstrate 320-W output power with 28% electrical-to-optical efficiency, which is, to our knowledge, the highest efficiency reported for diode-pumped solid-state lasers.  相似文献   

9.
165-W cryogenically cooled Yb:YAG laser   总被引:3,自引:0,他引:3  
Ripin DJ  Ochoa JR  Aggarwal RL  Fan TY 《Optics letters》2004,29(18):2154-2156
Thermo-optic distortions often limit the beam quality and power scaling of high-average-power lasers. Cryogenically cooled Yb:YAG is used to efficiently generate 165 W of near-diffraction-limited beam from a power oscillator with negligible thermo-optic effects. End pumped with 215 W of incident pump power from two diode modules, the laser has an optical-optical efficiency of 76%, a slope efficiency of 85%, and an M2 value of 1.02.  相似文献   

10.
Recent developments in high-finesse cavities now make broadly tunable, continuous-wave Raman lasers possible. The design and preliminary characterization of what is to the authors' knowledge the first continuous-wave Raman laser in H(2) are presented. The threshold is currently at 2 mW of pump, making diode laser pumping possible. The maximum photon conversion efficiency observed was 35% at 7.6 mW of pump power.  相似文献   

11.
Diode lasers are by far the most efficient lasers currently available. With the ever‐continuing improvement in diode laser technology, this type of laser has become increasingly attractive for a wide range of biomedical applications. Compared to the characteristics of competing laser systems, diode lasers simultaneously offer tunability, high‐power emission and compact size at fairly low cost. Therefore, diode lasers are increasingly preferred in important applications, such as photocoagulation, optical coherence tomography, diffuse optical imaging, fluorescence lifetime imaging, and terahertz imaging. This review provides an overview of the latest development of diode laser technology and systems and their use within selected biomedical applications. 670 nm external cavity diode laser for Raman spectroscopy built on a 13 × 4 mm2 microbench (Copyright FBH/Schurian.com ).  相似文献   

12.
The high efficient laser performance of self-Q-switched laser in the co-doped Cr4+,Nd3+:YAG microchip with 1.8 mm thickness was demonstrated. The slope efficiency is varied with the reflectivity of output coupler at 1064 nm, and the highest slope efficiency of 26% was obtained for 95% reflectivity of output coupler at 1064 nm. The pulse width, the single pulse energy and the pulse repetition rate for different reflectivity of the output couplers were measured, and the experimental results agree with the numerical calculations of the passively Q-switched rate equations. This can lead to develop the diode laser pumped monolithic self-Q-switched solid-state microchip lasers, especially for the intracavity frequency-doubled solid-state microchip lasers.  相似文献   

13.
Efficient and stable continuous-wave (CW) laser operation at 1053 nm in a Nd-doped phosphate single-mode fiber (Nd:PSMF) has been demonstrated experimentally. The fiber laser consisted of a 21 cm Nd:PSMF placed in a F-P cavity formed by high reflector butt-coupled to coupling end of the fiber and Fresnel reflection of the other end facet. An output power of 1.42 W and a slope efficiency of 34.1% (18.4%) with respect to absorbed pump power (incident pump power) were obtained with 808 nm diode pumping. An increment as much as 9.7 and 15.0% in slope efficiency of the input coupling efficiency and the output power, respectively, were obtained by using a local-cooling design provided by watered sealing the coupling point. The repeatable results indicate that the design, featuring fluid sealing the coupling point of the fiber laser, which was capable of offering an effective alleviation of thermal effects and an elevation of the quality of the laser cavity, could be expected to be a convenient and effective scheme to improve the performance characteristics of the non-silica fiber lasers and the high power fiber lasers, generally in free-space coupling configuration.  相似文献   

14.
Compact diode end-pumped acousto-optically Q-switched Nd:YLF laser was developed. As in effective CW diode end-pumped lasers, pump beam was made sufficiently narrower than resonator Gaussian mode to increase efficiency in Q-switched operation. The dramatic changes of output radiation structure were observed at some resonator lengths. The radiation structure is close to the Gaussian mode in intervals between these lengths.  相似文献   

15.
高功率半导体激光器在固体或光纤激光器泵浦、材料加工、医疗、传感、空间通讯和国防上有着极其重要的应用,但传统半导体激光器面临垂直发散角大、椭圆光斑的难题,限制了其直接应用。为了降低激光器的垂直发散角,本项目采用布拉格反射波导结构,利用光子带隙导引替代传统的全反射进行光场限制,优化设计了多种布拉格反射波导激光器结构,并制备了高性能的激光器器件。首先,采用传输矩阵理论和布洛赫波近似的方法计算了布拉格反射波导的模式色散关系,发现通过控制腔模光场分布,可实现不同远场的激光输出。接着,针对布拉格波导光子带隙导引机制,深入研究了四分之一波长布拉格反射波导激光器、单边布拉格反射波导激光器的光场特性,弄清了影响此类激光器远场的本质因素,最终设计并验证了一种布拉格反射波导双光束激光器,激光器在垂直方向可输出两个对称的、近圆形光束,单光束垂直和侧向发散角半高全宽分别低至7.2°和5.4°。另外,通过调控光缺陷层,使激光器工作在受抑隧穿光子带隙导引机制下,实现了超窄的单光束激光输出,激光器单管连续输出功率超过4.6 W,垂直发散角最低降至4.9°(半高全宽)和9.8°(95%功率)。这种高功率、窄的圆形光束输出可以大幅降低半导体激光器的应用成本,提高泵浦或光纤耦合效率,具有广阔的应用前景。  相似文献   

16.
We report on a diode-laser-pumped cw Nd: YAG laser operating at a power level of 150 W. By using a transverse pump geometry, the radiation of 54 diode lasers with an output power of 10 W each is coupled into a Nd:YAG rod. In multimode operation, an optical slope efficiency of 32% and an optical to optical efficiency of 29% are obtained. In TEM00 operation, an output power of more than 30 W is realized with an optical to optical efficiency of 10%.  相似文献   

17.
大功率半导体激光合束进展   总被引:1,自引:0,他引:1       下载免费PDF全文
王立军  彭航宇  张俊 《中国光学》2015,8(4):517-534
经过近30年的发展,半导体激光器已由信息器件逐步发展成为能量器件,特别是大功率高光束质量半导体激光器,已从泵浦光源过渡成为直接作用光源,并部分应用在加工及国防领域。本文介绍了大功率半导体激光单元发展现状,分析讨论了各种激光合束技术及相应的合束光源,介绍了长春光机所在激光合束方面所做的部分工作,提出了我国半导体激光产业建设及发展的几点建议,并对半导体激光技术的发展新动向进行了展望。随着单元亮度的提升和合束技术的成熟,大功率半导体激光源作为间接光源和直接作用光源将在国防和工业领域大放异彩。  相似文献   

18.
cw Raman lasing of Na2 molecules generated in a heated, sealed-off, all-sapphire cell is demonstrated. Being not damaged by highly corrosive alkaline vapours, this type of cell enables operation without buffer gas in contrast to the normal heatpipe operation of these lasers. This allows us to study Raman lasers in alkaline vapours in new regimes and under ideal conditions. With an argon ion pump laser at 488 nm, Raman laser operation at 525 nm with more than 10% efficiency and thresholds below 0.2 mW for a cell without buffer gas (length 9 cm) have been obtained so far. The low thresholds, being a factor of 10 less than for comparable heatpipe operation, gives us the chance to use low-power diode lasers as pump sources and to realize compact reliable Raman laser systems. Received: 17 May 1999 / Published online: 25 August 1999  相似文献   

19.
Efficiencies improvement of LD (laser diode) pumped multimode large mode area (LMA) Tm3+ doped double cladding silica fiber lasers with different in-line biconial tapers were reported. Two types of multimode Tm3+ doped fiber were used in this experiment. Each type of fiber was made into three fiber lasers, a uniform geometry fiber laser and two tapered fiber lasers with different taper parameters. Biconical tapers located several centimeters from the output end of the multimode fiber lasers were made by heating and stretching method. Although the threshold of the best tapered fiber laser was added 200 mW, the slope efficiency (25.3%) and the maximum output power (1.31 W) of the fiber laser increased by 10.3% and 350 mW respectively, in comparison with the un-tapered one. Pre and post output laser power ratio was 6.3–15.6. Simultaneously, the laser spectrum moved to shorter wavelengths. The same trends of these characteristics were also observed in the other three tapered fiber lasers.  相似文献   

20.
We demonstrate a nonresonant cw Raman laser pumped by an optically locked diode laser at 790 nm that produces cw Stokes (1178-nm) and coherent anti-Stokes (595-nm) emission. Considering the modest pump powers, relative low cost, and predicted spectral purity, we expect that frequency downconversion of tunable diode lasers through stimulated Raman scattering will provide an attractive source for remote sensing, spectroscopic, and atomic physics applications. The Stokes laser threshold is 240+/-19muW pump power, and emission is observed over a roughly 10-nm range by adjustment of the optical locking feedback phase. Photon-conversion efficiency rises throughout the pump-power region, with a peak value of 15+/-2% .  相似文献   

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