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基于三能级速率方程建立了横向泵浦铷蒸气激光器阈值计算模型,首次详细研究了横向泵浦铷蒸气激光器的泵浦阈值特性。论文结合实际参数,数值模拟了单Bar条半导体激光器横向泵浦铷蒸气的非线性吸收和泵浦光在蒸气室内的传播以及阈值工作状态下小信号增益的分布,仿真分析了蒸气室长度、温度、缓冲气体气压及组份配比、聚焦透镜焦距以及谐振腔诸参数对横向泵浦铷蒸气激光器出光阈值的影响。分析结果表明:对缓冲气体组份配比进行优化可以有效的降低泵浦阈值功率;蒸气室长度与温度共同影响阈值功率;较大的窗口片透过率和不大于70%的输出耦合率可以使泵浦阈值功率保持在较低的水平。文中对铷蒸气激光器等碱金属蒸气激光器的关键部件设计和系统优化可起到借鉴参考的作用。 相似文献
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环形腔掺铒光纤激光器的实验研究 总被引:3,自引:0,他引:3
利用掺饵光纤和环形腔结构,在980nm半导体激光器泵浦下,获得了1.56μm波长的光纤激光器输出。激光器的阈值泵浦功率为5.2mW。具有很好的线性输出特性。 相似文献
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用环形染料激光器观察并记录了腔内激光功率和激光频率随泵浦功率的变化。激光器在第一次达到阈值并建立激光振荡后,随着泵浦功率的增加先后出现第二、第三个阈值,激光功率出现两次不连续突变;同时激光器两次出现由单频工作到双频工作的跃变。 相似文献
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一般认为,光纤激光器模式不稳定效应主要来自于泵浦源量子亏损和增益光纤泵浦吸收所产生的热效应。理论分析了光纤中的热源,发现诱发模式不稳定的热效应主要来源于泵浦吸收、其次是量子亏损;利用课题组开发的仿真软件SeeFiberLaser对该结论进行仿真。仿真结果表明:泵浦吸收系数越低,光纤中的最高温度和温度梯度越低,越有利于抑制热致折射率光栅的形成,提高模式不稳定阈值。搭建了纤芯/包层直径为30/400 μm的前向泵浦掺镱光纤激光振荡器,对比研究了中心波长为976 nm 、915 nm和940 nm的泵浦源泵浦时激光器的模式不稳定阈值特性。结果表明,分别采用中心波长为976 nm 、915 nm和940 nm 的半导体激光器作为泵浦源时,激光器模式不稳定阈值分别为279 W、502 W和697 W,光光转化效率分别为67.7%、61%和63%。由此可以发现,泵浦吸收系数对模式不稳定阈值的影响大于量子亏损对模式不稳定阈值的影响,通过改变泵浦波长降低泵浦吸收系数可以有效提升模式不稳定阈值。优化泵浦波长,兼顾量子效率和泵浦吸收系数,是光纤激光器实现高光束质量高模式不稳定阈值的重要技术路线之一。 相似文献
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双包层光纤为利用大功率半导体激光列阵泵浦提供了一个解决途径,但是随着激光功率的
提高,光纤中斯托克斯光产生的振荡将会大大限制光纤激光器中激光功率的进一步提高。利用双包层
光纤激光器的速率传输方程,在忽略自发发射的情况下,对方程进行了近似的解析求解,得到斯托克
斯光达到阈值时,光纤中激光功率以及激光器泵浦功率的表达式。利用这些表达式,我们分析了阈值
泵浦功率与激光器参量(如光纤长度,掺杂浓度)的关系 相似文献
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An efficient, scalable, diode-pumped Nd laser design is reported. The gain element can be longitudinally pumped along five separate axes and is relatively simple to fabricate. Both Nd:YAG and Nd:YVO4 gain media were evaluated. Using five single-stripe laser diodes to pump the Nd:YAG, 3.94 W of absorbed power produced 2.1 W CW at 1.06 μm. The slope efficiency was 54 percent and the output was TEM00. The threshold power was 40 mW. No evidence of thermal saturation was observed up to the maximum pump power. Repetitively Q-switched operation is also reported. The maximum output power for Nd:YVO4 obtained with 2.9 W of pump power was 1.3 W. The slope efficiency was 47 percent 相似文献
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激光二极管端面泵浦的多晶Nd:YAG 1.32μm连续激光器 总被引:3,自引:0,他引:3
本文报道了激光二极管端面泵浦的多晶Nd:YAG(Polycrystalline Nd:YAG ceramic)1.32μm连续激光器的实验研究.在泵浦功率为2.1W时,激光达到阈值开始输出;在泵浦功率为9W时,输出功率达到690mW,斜率效率为11%.据我们所知,这是目前报道的功率最大的多晶Nd:YAGl.32μm连续激光器。 相似文献
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Pump power stability range of single-mode solid-state lasers with rod thermal lensing 总被引:1,自引:0,他引:1
The pump power stability range of solid-state laser resonators operating in the TEM00 mode has been thoroughly investigated. It has been shown that, for a very general resonator containing intracavity optical systems, rod thermal lensing engenders a pump power stability range which is a characteristic parameter of laser material and pump cavity, but is independent of resonator configuration. Stability ranges have been calculated and critically discussed for Nd:YAG, Nd:glasses, Nd: Cr: GSGG, and alexandrite. The independence of the pump power stability range from the resonator configuration has been experimentally demonstrated for a CW Nd:YAG laser. 相似文献
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基于石墨烯被动调Q Nd:YAG晶体微片激光器 总被引:1,自引:0,他引:1
设计了以石墨烯作为可饱和吸收体的被动调Q掺钕钇铝石榴石晶体(Nd:YAG)微片激光器。该激光器采用三明治结构,附有石墨烯薄层的YAG晶体紧密压贴于工作物质Nd:YAG晶体上,晶体端面镀膜作为端面镜构成平行平面谐振腔。采用光纤耦合输出激光二极管端面抽运技术,利用石墨烯的可饱和吸收作用,在注入功率为1.17 W时实现微片激光器的调Q运转,获得波长1064.6 nm,重复频率300~807 kHz可调,最小脉冲宽度75 ns的激光输出。激光器最大输出功率38.4 mW,最大单脉冲能量54.7 nJ。 相似文献
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Optimization of fiber-coupled laser-diode end-pumped lasers:influence of pump-beam quality 总被引:1,自引:0,他引:1
Chen Y.F. Liao T.S. Kao C.F. Huang T.M. Lin K.H. Wang S.C. 《Quantum Electronics, IEEE Journal of》1996,32(11):2010-2016
A general model has been developed for the optimization of fiber-coupled laser-diode pumped lasers by including the effect of pump-beam quality into the mode-overlap integrals. The numerical results of the mode-overlap integrals have been fitted to an analytical function of pump spot size, laser mode size and the parameter β, which is in terms of laser-diode beam quality and properties of the active medium. This analytical function allowed us to obtain explicit formulae for the threshold pump power, the slope efficiency, and the optimum pump spot size. With these formulae, the optimum mode size and the maximum output efficiency can be easily calculated for arbitrary values of β and input power. From the numerical results, we obtained an analytical expression to relate the required input power and pump-beam quality to the desired output efficiency and properties of an active medium. The present model provides a straightforward procedure to design the laser resonator and the optical coupling system for optimization. To illustrate the utility of the present model, a Nd:YAG laser pumped by fiber-coupled laser diodes is considered and optimized 相似文献
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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
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A scalable diode-pumped Nd:YAG laser is described in which the gain element resembles a penta-prism. This design allows longitudinal pumping along five separate axes. Using five high-power single stripe laser diodes, 4.16 W of absorbed power produced 2.3 W CW at 1.06 μm. The slope efficiency was 56%, the output was plane polarized, and the laser operated in the TEM00 mode. The threshold power, was 48 mW. No evidence of thermal saturation was observed up to the maximum pump power. With an intracavity KTP crystal, 431 mW of CW amplitude-stable output at 532 nm was generated. Repetitive Q-switched operation is also reported 相似文献
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设计了以石墨烯作为可饱和吸收体的被动调Q掺钕钇铝石榴石晶体(Nd∶YAG)微片激光器。该激光器采用三明治结构,附有石墨烯薄层的YAG晶体紧密压贴于工作物质Nd∶YAG晶体上,晶体端面镀膜作为端面镜构成平行平面谐振腔。采用光纤耦合输出激光二极管端面抽运技术,利用石墨烯的可饱和吸收作用,在注入功率为1.17W时实现微片激光器的调Q运转,获得波长1064.6nm,重复频率300~807kHz可调,最小脉冲宽度75ns的激光输出。激光器最大输出功率38.4mW,最大单脉冲能量54.7nJ。 相似文献
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Fedorov V.V. Mirov S.B. Gallian A. Badikov D.V. Frolov M.P. Korostelin Y.V. Kozlovsky V.I. Landman A.I. Podmar'kov Y.P. Akimov V.A. Voronov A.A. 《Quantum Electronics, IEEE Journal of》2006,42(9):907-917
Spectroscopic properties and lasing of Fe:ZnSe and co-doped Fe:Cr:ZnSe crystals in the mid-infrared spectral range were studied at room and low temperatures. Using a free-running Er:YAG laser as a pump source, the output energy of the thermoelectrically cooled Fe:ZnSe laser was 142 mJ with 30% slope efficiency at T=220 K. Passive Q-switched oscillation of Er:YAG laser with Fe:ZnSe crystal was demonstrated and used as a pump source for a Fe:ZnSe laser system. Room-temperature (RT) gain-switched lasing of Fe:ZnSe was achieved in microchip and selective cavity configurations using Q-switched Er:YAG and Raman-shifted Nd:YAG lasers as pump sources. The microchip laser threshold of 100 mJ/cm/sup 2/ was demonstrated using a Fe:ZnSe crystal without any reflection coatings. A slope efficiency of 13%, oscillation threshold of 1.3 mJ, and tunable oscillation of Fe:ZnSe laser systems over 3.95-5.05 /spl mu/m spectral range were realized at RT. 相似文献