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掺Yb光纤激光器抽运阈值研究 总被引:1,自引:0,他引:1
根据粒子数速率方程,石英中Yb^3 的能级和光谱特性及MucCumber关系式推导了描述掺Yb光纤激光器抽运阈值的表达式,对影响抽运 值的各因素进行了分析,并进行了相应的实验研究,理论值与实验结果符合。 相似文献
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报道了一种新型自倍频晶体Yb∶Gd0.2Y0.75(BO3)4(Yb∶GdYAB)在二极管激光器端面抽运条件下的连续光激光运转。为了实现紧凑的新型全固态激光器的激光运转,设计了一个平平谐振腔,两个镜子的分开距离仅为1 cm,在这种腔结构下,得到了中心波长为1044 nm的基频激光输出,当吸收抽运功率为4.22 W时,基频激光的最大输出功率为1.38 W,相应功率曲线最大斜效率为54%。为获得有效的自倍频激光输出,换用了平凹腔进行了自倍频实验。自倍频光运转阈值仅为900 mW,在吸收抽运功率为3.9 W的条件下,得到144 mW的自倍频绿色激光输出,获得从二极管激光器到绿光的直接光-光转换效率为3.7%。实验结果表明Yb∶GdYAB作为一种新型的自倍频晶体,对于紧凑的1μm波段的基频光和自倍频可见光激光器都有着很大的应用潜力。 相似文献
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掺Yb光纤激光器激射波长与阈值关系研究 总被引:6,自引:0,他引:6
依据石英中 Yb3 的能级和光谱特性 ,推导了掺 Yb光纤激光器中激射波长与抽运阈值等的关系式。依据所得到的关系式 ,深入分析、研究了抽运功率、损耗及阈值对激光运行波长的影响。进行了相关实验 ,理论与实验结果符合得很好 相似文献
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线阵激光二极管侧面抽运Nd∶YAG激光器特性研究 总被引:1,自引:0,他引:1
依据四能级系统速率方程 ,推导出了多横模振荡固体激光器输出与输入参量的关系。对二极管抽运固体激光器中线阵激光二极管三向对称侧面抽运结构 ,计算了抽运光强分布 ,并就激光器的阈值抽运功率、近阈值条件下的斜率效率、输出功率和光束质量等与抽运参量的关系 ,进行了数值计算。由计算结果看出 ,线阵激光二极管侧面抽运Nd∶YAG激光器中晶体半径和抽运光束腰半径是影响输出激光功率和光束质量的主要因素 ,并通过在谐振腔中加小孔选模 ,使光束质量得到明显改善。选择了一组三向侧面抽运结构参量进行了实验验证 ,实验结果与理论计算一致。 相似文献
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线阵激光二极管侧面抽运Nd:YAG激光器特性研究 总被引:8,自引:2,他引:6
依据四能级系统速率方程,推导出了多横模振荡固体激光器输出与输入参量的关系。对二极管抽运固体激光器中线阵激光二极管三向对称侧面抽运结构,计算了抽运光强分布,并就激光器的阈值抽运功率、近阈值条件下的斜率效率、输出功率和光束质量等与抽运参量的关系,进行了数值计算。由计算结果看出,线阵激光二极管侧面抽运Nd:YAG激光器中晶体半径和抽运光束腰半径是影响输出激光功率和光束质量的主要因素,并通过在谐振腔中加小孔选模,使光束质量得到明显改善。选择了一组三向侧面抽运结构参量进行了实验验证,实验结果与理论计算一致。 相似文献
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端-侧面组合抽运方案是提高DPL调Q脉冲峰值功率和压缩脉冲宽度的有效技术途径。借助给出的一组端-侧面组合抽运DPL声光调Q实验结果,依据调Q速率方程,理论分析了组合抽运光的空间分布对调Q脉冲特性的影响,数值计算结果与实验结果一致。实验和理论研究发现:组合抽运时的脉冲宽度明显小于侧面抽运时的脉冲宽度,峰值功率明显高于侧面抽运时的峰值功率。实验和分析结果表明:在总抽运功率和抽运结构确定的情况下,端面抽运光功率在总抽运功率中的占有率越大,脉冲宽度越窄,脉冲峰值功率越高。通过调整端面抽运光功率占有率,改变组合抽运光的空间分布,可以实现对DPL调Q脉冲特性的控制。 相似文献
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A new model on quasi-three-level end-pumped CW Yb:YAG lasers is proposed. The presented model is expected and proved to be more accurate than previously published works on this subject as it is capable of dealing with end-pumped laser systems in the situation that non-uniform longitudinal temperature distribution exists along the laser rod, which is in fact always be true. To illustrate the utility of the derived equations, a diode end-pumped kilowatt class CW Yb:YAG laser is examined. By comparing with the former study, the presented model shows output power reductions of about 15.7 and 8.9% for single- and double-pass pumping geometries, respectively. 相似文献
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The absorption and fluorescence spectra of Cr,Yb:YAG crystal were measured. There are two absorption bands at 940 nm and 968 nm although the absorption coefficient is lower than that of the absorption peak of Yb:YAG superimposed in Cr:YAG absorption peak. The emission peak intensity is 4 times lower than that of Yb:YAG, which may be caused by the existence of the ground state absorption of Cr4+ which quenches the Yb3+ emission intensity. Although the emission peak of Cr,Yb:YAG is lower than that of Yb:YAG, there is an advantage of this crystal which combines the saturable absorber and gain medium into one and can be a self-Q switching laser crystal if Cr,Yb:YAG crystal is pumped with high energy power. 相似文献
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本文通过分析不同泵浦功率密度下类钾硅离子X射线激光的实验结果以及有可能实现X射线激光的其它类锂离子的光谱特性,表明利用类锂离子复合方案,在现有驱动激光装置上实现“水窗”波段放大器有很大的可能性。 相似文献
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M. V. Bogdanovich A. I. Enzhievskii G. I. Ryabtsev V. V. Kuznetsova V. V. Mashko L. L. Teplyashin L. I. Burov A. G. Ryabtsev M. A. Shchemelev A. S. Kraskovskii 《Journal of Applied Spectroscopy》2006,73(4):546-550
Based on analysis of the laser emission spectra of borosilicophosphate glass, coactivated by Er3+ and Yb3+ ions, we have determined the structure of the Stark splitting of the luminescence band for the erbium ion in the 1.5 μm region
(the transition 4I13/2 → 4I15/2). In the wavelength interval 1532–1547 nm, we identified 12 sets of lines belonging to different types of optical centers
of predominantly cubic symmetry.
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Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 73, No. 4, pp. 483–487, July–August, 2006. 相似文献
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A Nd:CNGG laser operated at 935 nm and 1061 nm pumped at 885 nm and 808 nm, respectively, is demonstrated. The 885 nm direct pumping scheme shows some advantages over the 808 nm traditional pumping scheme. It includes higher slope efficiency, lower threshold, and better beam quality at high output power. With the direct pumping, the slope efficiency increases by 43% and the threshold decreases by 10% compared with traditional pumping in the Nd:CNGG laser operated at 935 nm. When the Nd:CNGG laser operates at 1061 nm, the direct pumping increases the slope efficiency by 14% with a 20% reduction in the oscillation threshold. 相似文献